Optical image capturing system

ABSTRACT

A six-piece optical lens for capturing image and a six-piece optical module for capturing image are provided. In order from an object side to an image side, the optical lens along the optical axis includes a first lens with refractive power, a second lens with refractive power, a third lens with refractive power, a fourth lens with refractive power, a fifth lens with refractive power and a sixth lens with refractive power. At least one of the image-side surface and object-side surface of each of the six lens elements is aspheric. The optical lens can increase aperture value and improve the imagining quality for use in compact cameras.

CROSS-REFERENCE TO RELATED APPLICATION

This application claims the benefit of Taiwan Patent Application No.104129229, filed on Sep. 3, 2015, in the Taiwan Intellectual PropertyOffice, the disclosure of which is incorporated herein in its entiretyby reference.

BACKGROUND OF THE INVENTION 1. Field of the Invention

The present disclosure relates to an optical image capturing system, andmore particularly to a compact optical image capturing system which canbe applied to electronic products.

2. Description of the Related Art

In recent years, with the rise of portable electronic devices havingcamera functionalities, the demand for an optical image capturing systemis raised gradually. The image sensing device of ordinary photographingcamera is commonly selected from charge coupled device (CCD) orcomplementary metal-oxide semiconductor sensor (CMOS Sensor). Inaddition, as advanced semiconductor manufacturing technology enables theminimization of pixel size of the image sensing device, the developmentof the optical image capturing system directs towards the field of highpixels. Therefore, the requirement for high imaging quality is rapidlyraised.

The traditional optical image capturing system of a portable electronicdevice comes with different designs, including a four-lens or afive-lens design. However, the requirement for the higher pixels and therequirement for a large aperture of an end user, like functionalities ofmicro filming and night view, or the requirement of wide view angle ofthe portable electronic device have been raised. But the optical imagecapturing system with the large aperture design often produces moreaberration resulting in the deterioration of quality in peripheral imageformation and difficulties of manufacturing, and the optical imagecapturing system with wide view angle design increases distortion ratein image formation, thus the optical image capturing system in priorarts cannot meet the requirement of the higher order camera lens module.

Therefore, how to effectively increase quantity of incoming light andview angle of the optical lenses, not only further improves total pixelsand imaging quality for the image formation, but also considers theequity design of the miniaturized optical lenses, becomes a quiteimportant issue.

SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an opticalimage capturing system and an optical image capturing lens which usecombination of refractive powers, convex and concave surfaces ofsix-piece optical lenses (the convex or concave surface in thedisclosure denotes the geometrical shape of an image-side surface or anobject-side surface of each lens on an optical axis) to increase thequantity of incoming light of the optical image capturing system and theview angle of the optical lenses, and to improve total pixels andimaging quality for image formation, so as to be applied to minimizedelectronic products.

The term and its definition to the lens element parameter in theembodiment of the present invention are shown as below for furtherreference.

The Lens Element Parameter Related to a Length or a Height in the LensElement

A maximum height for image formation of the optical image capturingsystem is denoted by HOI. A height of the optical image capturing systemis denoted by HOS. A distance from the object-side surface of the firstlens element to the image-side surface of the sixth lens element isdenoted by InTL. A distance from an aperture stop (aperture) to an imageplane is denoted by InS. A distance from the first lens element to thesecond lens element is denoted by In12 (instance). A central thicknessof the first lens element of the optical image capturing system on theoptical axis is denoted by TP1 (instance).

The Lens Element Parameter Related to a Material in the Lens Element

An Abbe number of the first lens element in the optical image capturingsystem is denoted by NA1 (instance). A refractive index of the firstlens element is denoted by Nd1 (instance).

The Lens Element Parameter Related to a View Angle in the Lens Element

A view angle is denoted by AF. Half of the view angle is denoted by HAF.A major light angle is denoted by MRA.

The Lens Element Parameter Related to Exit/Entrance Pupil in the LensElement

An entrance pupil diameter of the optical image capturing system isdenoted by HEP. A maximum effective half diameter (EHD) of any surfaceof a single lens element refers to a perpendicular height between anintersection point on the surface of the lens element where the incidentlight with the maximum view angle in the optical system passes throughthe outmost edge of the entrance pupil and the optical axis. Forexample, the maximum effective half diameter of the object-side surfaceof the first lens element is denoted by EHD 11. The maximum effectivehalf diameter of the image-side surface of the first lens element isdenoted by EHD 12. The maximum effective half diameter of theobject-side surface of the second lens element is denoted by EHD 21. Themaximum effective half diameter of the image-side surface of the secondlens element is denoted by EHD 22. The maximum effective half diametersof any surfaces of other lens elements in the optical image capturingsystem are denoted in the similar way.

The Lens Element Parameter Related to a Depth of the Lens Element Shape

A distance in parallel with an optical axis from a maximum effectivediameter position to an axial point on the object-side surface of thesixth lens element is denoted by InRS61 (instance). A distance inparallel with an optical axis from a maximum effective diameter positionto an axial point on the image-side surface of the sixth lens element isdenoted by InRS62 (instance).

The Lens Element Parameter Related to the Lens Element Shape

A critical point C is a tangent point on a surface of a specific lenselement, and the tangent point is tangent to a plane perpendicular tothe optical axis and the tangent point cannot be a crossover point onthe optical axis. To follow the past, a distance perpendicular to theoptical axis between a critical point C51 on the object-side surface ofthe fifth lens element and the optical axis is HVT51 (instance). Adistance perpendicular to the optical axis between a critical point C52on the image-side surface of the fifth lens element and the optical axisis HVT52 (instance). A distance perpendicular to the optical axisbetween a critical point C61 on the object-side surface of the sixthlens element and the optical axis is HVT61 (instance). A distanceperpendicular to the optical axis between a critical point C62 on theimage-side surface of the sixth lens element and the optical axis isHVT62 (instance). Distances perpendicular to the optical axis betweencritical points on the object-side surfaces or the image-side surfacesof other lens elements and the optical axis are denoted in the similarway described above.

The object-side surface of the sixth lens element has one inflectionpoint IF611 which is nearest to the optical axis, and the sinkage valueof the inflection point IF611 is denoted by SGI611 (instance). SGI611 isa horizontal shift distance in parallel with the optical axis from anaxial point on the object-side surface of the sixth lens element to theinflection point which is nearest to the optical axis on the object-sidesurface of the sixth lens element. A distance perpendicular to theoptical axis between the inflection point IF611 and the optical axis isHIF611 (instance). The image-side surface of the sixth lens element hasone inflection point IF621 which is nearest to the optical axis and thesinkage value of the inflection point IF621 is denoted by SGI621(instance). SGI621 is a horizontal shift distance in parallel with theoptical axis from an axial point on the image-side surface of the sixthlens element to the inflection point which is nearest to the opticalaxis on the image-side surface of the sixth lens element. A distanceperpendicular to the optical axis between the inflection point IF621 andthe optical axis is HIF621 (instance).

The object-side surface of the sixth lens element has one inflectionpoint IF612 which is the second nearest to the optical axis and thesinkage value of the inflection point IF612 is denoted by SGI612(instance). SGI612 is a horizontal shift distance in parallel with theoptical axis from an axial point on the object-side surface of the sixthlens element to the inflection point which is the second nearest to theoptical axis on the object-side surface of the sixth lens element. Adistance perpendicular to the optical axis between the inflection pointIF612 and the optical axis is HIF612 (instance). The image-side surfaceof the sixth lens element has one inflection point IF622 which is thesecond nearest to the optical axis and the sinkage value of theinflection point IF622 is denoted by SGI622 (instance). SGI622 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theinflection point which is the second nearest to the optical axis on theimage-side surface of the sixth lens element. A distance perpendicularto the optical axis between the inflection point IF622 and the opticalaxis is HIF622 (instance).

The object-side surface of the sixth lens element has one inflectionpoint IF613 which is the third nearest to the optical axis and thesinkage value of the inflection point IF613 is denoted by SGI613(instance). SGI613 is a horizontal shift distance in parallel with theoptical axis from an axial point on the object-side surface of the sixthlens element to the inflection point which is the third nearest to theoptical axis on the object-side surface of the sixth lens element. Adistance perpendicular to the optical axis between the inflection pointIF613 and the optical axis is HIF613 (instance). The image-side surfaceof the sixth lens element has one inflection point IF623 which is thethird nearest to the optical axis and the sinkage value of theinflection point IF623 is denoted by SGI623 (instance). SGI623 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theinflection point which is the third nearest to the optical axis on theimage-side surface of the sixth lens element. A distance perpendicularto the optical axis between the inflection point IF623 and the opticalaxis is HIF623 (instance).

The object-side surface of the sixth lens element has one inflectionpoint IF614 which is the fourth nearest to the optical axis and thesinkage value of the inflection point IF614 is denoted by SGI14(instance). SGI614 is a horizontal shift distance in parallel with theoptical axis from an axial point on the object-side surface of the sixthlens element to the inflection point which is the fourth nearest to theoptical axis on the object-side surface of the sixth lens element. Adistance perpendicular to the optical axis between the inflection pointIF614 and the optical axis is HIF614 (instance). The image-side surfaceof the sixth lens element has one inflection point IF624 which is thefourth nearest to the optical axis and the sinkage value of theinflection point IF624 is denoted by SGI624 (instance). SGI624 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theinflection point which is the fourth nearest to the optical axis on theimage-side surface of the sixth lens element. A distance perpendicularto the optical axis between the inflection point IF624 and the opticalaxis is HIF624 (instance).

The inflection points on the object-side surfaces or the image-sidesurfaces of the other lens elements and the distances perpendicular tothe optical axis thereof or the sinkage values thereof are denoted inthe similar way described above.

The Lens Element Parameter Related to an Aberration

Optical distortion for image formation in the optical image capturingsystem is denoted by ODT. TV distortion for image formation in theoptical image capturing system is denoted by TDT. Further, the range ofthe aberration offset for the view of image formation may be limited to50%-100%. An offset of the spherical aberration is denoted by DFS. Anoffset of the coma aberration is denoted by DFC.

The vertical coordinate axis of the characteristic diagram of modulationtransfer function represents a contrast transfer rate (values are from 0to 1). The horizontal coordinate axis represents a spatial frequency(cycles/mm; lp/mm; line pairs per mm). Theoretically, an ideal imagecapturing system can 100% show the line contrast of a photographedobject. However, the values of the contrast transfer rate at thevertical coordinate axis are smaller than 1 in the actual imagecapturing system. The transfer rate of its comparison value is less thana vertical axis. In addition, comparing to the central region, it isgenerally more difficult to achieve a fine degree of recovery in theedge region of image capturing. The contrast transfer rates (MTF values)with spatial frequencies of 55 cycles/m at the optical axis, 0.3 fieldof view and 0.7 field of view of a visible spectrum on the image planeare respectively denoted by MTFE0, MTFE3 and MTFE7. The contrasttransfer rates (MTF values) with spatial frequencies of 110 cycles/m atthe optical axis, 0.3 field of view and 0.7 field of view on the imageplane are respectively denoted by MTFQ0, MTFQ3 and MTFQ7. The contrasttransfer rates (MTF values) with spatial frequencies of 220 cycles/m atthe optical axis, 0.3 field of view and 0.7 field of view on the imageplane are respectively denoted by MTFH0, MTFH3 and MTFH7. The contrasttransfer rates (MTF values) with spatial frequencies of 440 cycles/m atthe optical axis, 0.3 field of view and 0.7 field of view on the imageplane are respectively denoted by MTF0, MTF3 and MTF7. The three fieldsof view described above are representative to the centre, the internalfield of view and the external field of view of the lens elements. Thus,they may be used to evaluate whether the performance of a specificoptical image capturing system is excellent. The design of the opticalimage capturing system of the present invention mainly corresponds to apixel size in which a sensing device below 1.12 micrometers is includes.Therefore, the quarter spatial frequencies, the half spatial frequencies(half frequencies) and the full spatial frequencies (full frequencies)of the characteristic diagram of modulation transfer functionrespectively are at least 110 cycles/mm, 220 cycles/mm and 440cycles/mm.

If an optical image capturing system needs to satisfy with the imagesaimed to infrared spectrum, such as the requirement for night visionwith lower light source, the used wavelength may be 850 nm or 800 nm. Asthe main function is to recognize shape of an object formed inmonochrome and shade, the high resolution is unnecessary, and thus, aspatial frequency, which is less than 100 cycles/mm, is used to evaluatethe functionality of the optical image capturing system, when theoptical image capturing system is applied to the infrared spectrum. Whenthe foregoing wavelength 850 nm is applied to focus on the image plane,the contrast transfer rates (MTF values) with a spatial frequency of 55cycles/mm at the optical axis, 0.3 field of view and 0.7 field of viewon the image plane are respectively denoted by MTFI0, MTFI3 and MTFI7.However, the infrared wavelength of 850 nm or 800 nm may be hugelydifferent to wavelength of the regular visible light wavelength, andthus, it is hard to design an optical image capturing system which hasto focus on the visible light and the infrared light (dual-mode)simultaneously while achieve a certain function respectively.

The disclosure provides an optical image capturing system, which is ableto focus on the visible light and the infrared light (dual-mode)simultaneously while achieve a certain function respectively, and anobject-side surface or an image-side surface of the fourth lens elementhas inflection points, such that the angle of incidence from each fieldof view to the fourth lens element can be adjusted effectively and theoptical distortion and the TV distortion can be corrected as well.Besides, the surfaces of the fourth lens element may have a betteroptical path adjusting ability to acquire better imaging quality.

The disclosure provides an optical image capturing system, in order froman object side to an image side, including a first, second, third,fourth, fifth, sixth lens elements and an image plane. The first lenselement has refractive power. An object-side surface and an image-sidesurface of the sixth lens element are aspheric. Focal lengths of thefirst through sixth lens elements are f1, f2, f3, f4, f5 and f6respectively. A focal length of the optical image capturing system is f.An entrance pupil diameter of the optical image capturing system is HEP.A distance from an object-side surface of the first lens element to theimage plane is HOS. Thicknesses in parallel with an optical axis of thefirst through sixth lens elements at height ½ HEP respectively are ETP1,ETP2, ETP3, ETP4, ETP5 and ETP6. A sum of ETP1 to ETP6 described aboveis SETP. Thicknesses of the first through sixth lens elements on theoptical axis respectively are TP1, TP2, TP3, TP4, TP5 and TP6. A sum ofTP1 to TP6 described above is STP. The following relations aresatisfied: 1.2≤f/HEP≤10.0 and 0.5≤SETP/STP<1.

The disclosure provides another optical image capturing system, in orderfrom an object side to an image side, including a first, second, third,fourth, fifth, sixth lens elements and an image plane. The first lenselement has negative refractive power, and the position near the opticalaxis on an object-side surface of the first lens element may be a convexsurface. The second lens element has refractive power. The third lenselement has refractive power. The fourth lens element has refractivepower. The fifth lens element has refractive power. The sixth lenselement has refractive power, and an object-side surface and animage-side surface of the sixth lens element are aspheric. A maximumheight for image formation on the image plane perpendicular to theoptical axis in the optical image capturing system is denoted by HOI,and at least one lens element among the first through the sixth lenselements is made of glass material. At least one of the second throughsixth lens elements has positive refractive power. Focal lengths of thefirst through sixth lens elements are f1, f2, f3, f4, f5 and f6respectively. A focal length of the optical image capturing system is f.An entrance pupil diameter of the optical image capturing system is HEP.A distance from an object-side surface of the first lens element to theimage plane is HOS. A horizontal distance in parallel with the opticalaxis from a coordinate point on the object-side surface of the firstlens element at height ½ HEP to the image plane is ETL. A horizontaldistance in parallel with the optical axis from a coordinate point onthe object-side surface of the first lens element at height ½ HEP to acoordinate point on the image-side surface of the sixth lens element atheight ½ HEP is EIN. The following relations are satisfied:1.2≤f/HEP≤10.0, HOI>3.0 mm and 0.2≤EIN/ETL<1.

The disclosure provides another optical image capturing system, in orderfrom an object side to an image side, including a first, second, third,fourth, fifth, sixth lens elements and an image plane. Wherein theoptical image capturing system consists of six lens elements withrefractive power, a maximum height for image formation on the imageplane perpendicular to the optical axis in the optical image capturingsystem is denoted by HOI, and at least three lens elements among thefirst through the sixth lens elements are made of glass material. Anobject-side surface and an image-side surface of at least one lenselement of the six lens elements are aspheric. At least one of the firstthrough sixth lens elements respectively has at least one inflectionpoint on at least one surface thereof. The first lens element hasnegative refractive power. The second lens element has refractive power.The third lens element has refractive power. The fourth lens element hasrefractive power. The fifth lens element has refractive power. The sixthlens element has refractive power. Focal lengths of the first throughsixth lens elements are f1, f2, f3, f4, f5 and f6 respectively. A focallength of the optical image capturing system is f. An entrance pupildiameter of the optical image capturing system is HEP. A half of maximumview angle of the optical image capturing system is HAF. A distance froman object-side surface of the first lens element to the image plane isHOS. A horizontal distance in parallel with the optical axis from acoordinate point on the object-side surface of the first lens element atheight ½ HEP to the image plane is ETL. A horizontal distance inparallel with the optical axis from a coordinate point on theobject-side surface of the first lens element at height ½ HEP to acoordinate point on the image-side surface of the sixth lens element atheight ½ HEP is EIN. The following relations are satisfied:1.2≤f/HEP≤3.0, 0.4≤|tan(HAF)|≤6.0, HOI>3.0 mm and 0.2≤EIN/ETL<1.

A thickness of a single lens element at height of ½ entrance pupildiameter (HEP) particularly affects the corrected aberration of commonarea of each field of view of light and the capability of correctingoptical path difference between each field of view of light in the scopeof ½ entrance pupil diameter (HEP). The capability of aberrationcorrection is enhanced if the thickness becomes greater, but thedifficulty for manufacturing is also increased at the same time.Therefore, it is necessary to control the thickness of a single lenselement at height of ½ entrance pupil diameter (HEP), in particular tocontrol the ratio relation (ETP/TP) of the thickness (ETP) of the lenselement at height of ½ entrance pupil diameter (HEP) to the thickness(TP) of the lens element to which the surface belongs on the opticalaxis. For example, the thickness of the first lens element at height of½ entrance pupil diameter (HEP) is denoted by ETP1. The thickness of thesecond lens element at height of ½ entrance pupil diameter (HEP) isdenoted by ETP2. The thicknesses of other lens elements are denoted inthe similar way. A sum of ETP1 to ETP6 described above is SETP. Theembodiments of the present invention may satisfy the following relation:0.3≤SETP/EIN<1.

In order to enhance the capability of aberration correction and reducethe difficulty for manufacturing at the same time, it is particularlynecessary to control the ratio relation (ETP/TP) of the thickness (ETP)of the lens element at height of ½ entrance pupil diameter (HEP) to thethickness (TP) of the lens element on the optical axis lens. Forexample, the thickness of the first lens element at height of ½ entrancepupil diameter (HEP) is denoted by ETP1. The thickness of the first lenselement on the optical axis is TP1. The ratio between both of them isETP1/TP1. The thickness of the second lens element at height of ½entrance pupil diameter (HEP) is denoted by ETP2. The thickness of thesecond lens element on the optical axis is TP2. The ratio between bothof them is ETP2/TP2. The ratio relations of the thicknesses of otherlens element in the optical image capturing system at height of ½entrance pupil diameter (HEP) to the thicknesses (TP) of the lenselements on the optical axis lens are denoted in the similar way. Theembodiments of the present invention may satisfy the following relation:0.2≤ETP/TP≤3.

A horizontal distance between two adjacent lens elements at height of ½entrance pupil diameter (HEP) is denoted by ED. The horizontal distance(ED) described above is in parallel with the optical axis of the opticalimage capturing system and particularly affects the corrected aberrationof common area of each field of view of light and the capability ofcorrecting optical path difference between each field of view of lightat the position of ½ entrance pupil diameter (HEP). The capability ofaberration correction may be enhanced if the horizontal distance becomesgreater, but the difficulty for manufacturing is also increased and thedegree of ‘miniaturization’ to the length of the optical image capturingsystem is restricted. Thus, it is essential to control the horizontaldistance (ED) between two specific adjacent lens elements at height of ½entrance pupil diameter (HEP).

In order to enhance the capability of aberration correction and reducethe difficulty for ‘miniaturization’ to the length of the optical imagecapturing system at the same time, it is particularly necessary tocontrol the ratio relation (ED/IN) of the horizontal distance (ED)between the two adjacent lens elements at height of ½ entrance pupildiameter (HEP) to the horizontal distance (IN) between the two adjacentlens elements on the optical axis. For example, the horizontal distancebetween the first lens element and the second lens element at height of½ entrance pupil diameter (HEP) is denoted by ED12. The horizontaldistance between the first lens element and the second lens element onthe optical axis is IN12. The ratio between both of them is ED12/IN12.The horizontal distance between the second lens element and the thirdlens element at height of ½ entrance pupil diameter (HEP) is denoted byED23. The horizontal distance between the second lens element and thethird lens element on the optical axis is IN23. The ratio between bothof them is ED23/IN23. The ratio relations of the horizontal distancesbetween other two adjacent lens elements in the optical image capturingsystem at height of ½ entrance pupil diameter (HEP) to the horizontaldistances between the two adjacent lens elements on the optical axis aredenoted in the similar way.

A horizontal distance in parallel with the optical axis from acoordinate point on the image-side surface of the sixth lens element atheight ½ HEP to the image plane is EBL. A horizontal distance inparallel with the optical axis from an axial point on the image-sidesurface of the sixth lens element to the image plane is BL. Theembodiments of the present invention enhance the capability ofaberration correction and reserve space for accommodating other opticalelements. The following relation may be satisfied: 0.2≤EBL/BL<1.1. Theoptical image capturing system may further include a light filtrationelement. The light filtration element is located between the sixth lenselement and the image plane. A distance in parallel with the opticalaxis from a coordinate point on the image-side surface of the sixth lenselement at height ½ HEP to the light filtration element is EIR. Adistance in parallel with the optical axis from an axial point on theimage-side surface of the sixth lens element to the light filtrationelement is PIR. The embodiments of the present invention may satisfy thefollowing relation: 0.1≤EIR/PIR≤1.1.

The height of optical system (HOS) may be reduced to achieve theminimization of the optical image capturing system when the absolutevalue of f1 is larger than f6 (|f1|>f6).

When |f2|+|f3|+|f4|+|f5| and |f1|+|f6| are satisfied with aboverelations, at least one of the second through fifth lens elements mayhave weak positive refractive power or weak negative refractive power.The weak refractive power indicates that an absolute value of the focallength of a specific lens element is greater than 10. When at least oneof the second through fifth lens elements has the weak positiverefractive power, the positive refractive power of the first lenselement can be shared, such that the unnecessary aberration will notappear too early. On the contrary, when at least one of the secondthrough fifth lens elements has the weak negative refractive power, theaberration of the optical image capturing system can be corrected andfine tuned.

The sixth lens element may have negative refractive power and a concaveimage-side surface. Hereby, the back focal length is reduced for keepingthe miniaturization, to miniaturize the lens element effectively. Inaddition, at least one of the object-side surface and the image-sidesurface of the sixth lens element may have at least one inflectionpoint, such that the angle of incident with incoming light from anoff-axis field of view can be suppressed effectively and the aberrationin the off-axis field of view can be corrected further.

BRIEF DESCRIPTION OF THE DRAWINGS

The detailed structure, operating principle and effects of the presentdisclosure will now be described in more details hereinafter withreference to the accompanying drawings that show various embodiments ofthe present disclosure as follows.

FIG. 1A is a schematic view of the optical image capturing systemaccording to the first embodiment of the present application.

FIG. 1B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the first embodimentof the present application.

FIG. 1C is a characteristic diagram of modulation transfer of a visiblelight according to the first embodiment of the present application.

FIG. 1D is a characteristic diagram of modulation transfer of infraredrays according to the first embodiment of the present application.

FIG. 2A is a schematic view of the optical image capturing systemaccording to the second embodiment of the present application.

FIG. 2B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the secondembodiment of the present application.

FIG. 2C is a characteristic diagram of modulation transfer of a visiblelight according to the second embodiment of the present application.

FIG. 2D is a characteristic diagram of modulation transfer of infraredrays according to the second embodiment of the present application.

FIG. 3A is a schematic view of the optical image capturing systemaccording to the third embodiment of the present application.

FIG. 3B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the third embodimentof the present application.

FIG. 3C is a characteristic diagram of modulation transfer of a visiblelight according to the third embodiment of the present application.

FIG. 3D is a characteristic diagram of modulation transfer of infraredrays according to the third embodiment of the present application.

FIG. 4A is a schematic view of the optical image capturing systemaccording to the fourth embodiment of the present application.

FIG. 4B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the fourthembodiment of the present application.

FIG. 4C is a characteristic diagram of modulation transfer of a visiblelight according to the fourth embodiment of the present application.

FIG. 4D is a characteristic diagram of modulation transfer of infraredrays according to the fourth embodiment of the present application.

FIG. 5A is a schematic view of the optical image capturing systemaccording to the fifth embodiment of the present application.

FIG. 5B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the fifth embodimentof the present application.

FIG. 5C is a characteristic diagram of modulation transfer of a visiblelight according to the fifth embodiment of the present application.

FIG. 5D is a characteristic diagram of modulation transfer of infraredrays according to the fifth embodiment of the present application.

FIG. 6A is a schematic view of the optical image capturing systemaccording to the sixth embodiment of the present application.

FIG. 6B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the sixth embodimentof the present application.

FIG. 6C is a characteristic diagram of modulation transfer of a visiblelight according to the sixth embodiment of the present application.

FIG. 6D is a characteristic diagram of modulation transfer of infraredrays according to the sixth embodiment of the present application.

FIG. 7A is a schematic view of the optical image capturing systemaccording to the seventh embodiment of the present application.

FIG. 7B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the seventhembodiment of the present application.

FIG. 7C is a characteristic diagram of modulation transfer of a visiblelight according to the seventh embodiment of the present application.

FIG. 7D is a characteristic diagram of modulation transfer of infraredrays according to the seventh embodiment of the present application.

FIG. 8A is a schematic view of the optical image capturing systemaccording to the eighth embodiment of the present application.

FIG. 8B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the eighthembodiment of the present application.

FIG. 8C is a characteristic diagram of modulation transfer of a visiblelight according to the eighth embodiment of the present application.

FIG. 8D is a characteristic diagram of modulation transfer of infraredrays according to the eighth embodiment of the present application.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Reference will now be made in detail to the exemplary embodiments of thepresent disclosure, examples of which are illustrated in theaccompanying drawings. Therefore, it is to be understood that theforegoing is illustrative of exemplary embodiments and is not to beconstrued as limited to the specific embodiments disclosed, and thatmodifications to the disclosed exemplary embodiments, as well as otherexemplary embodiments, are intended to be included within the scope ofthe appended claims. These embodiments are provided so that thisdisclosure will be thorough and complete, and will fully convey theinventive concept to those skilled in the art. The relative proportionsand ratios of elements in the drawings may be exaggerated or diminishedin size for the sake of clarity and convenience in the drawings, andsuch arbitrary proportions are only illustrative and not limiting in anyway. The same reference numbers are used in the drawings and thedescription to refer to the same or like parts.

It will be understood that, although the terms ‘first’, ‘second’,‘third’, etc., may be used herein to describe various elements, theseelements should not be limited by these terms. The terms are used onlyfor the purpose of distinguishing one component from another component.Thus, a first element discussed below could be termed a second elementwithout departing from the teachings of embodiments. As used herein, theterm “or” includes any and all combinations of one or more of theassociated listed items.

An optical image capturing system, in order from an object side to animage side, includes a first, second, third, fourth, fifth and sixthlens elements with refractive power and an image plane. The opticalimage capturing system may further include an image sensing device whichis disposed on an image plane.

The optical image capturing system may use three sets of wavelengthswhich are 486.1 nm, 587.5 nm and 656.2 nm, respectively, wherein 587.5nm is served as the primary reference wavelength and a referencewavelength for retrieving technical features. The optical imagecapturing system may also use five sets of wavelengths which are 470 nm,510 nm, 555 nm, 610 nm and 650 nm, respectively, wherein 555 nm isserved as the primary reference wavelength and a reference wavelengthfor retrieving technical features.

A ratio of the focal length f of the optical image capturing system to afocal length fp of each of lens elements with positive refractive poweris PPR. A ratio of the focal length f of the optical image capturingsystem to a focal length fn of each of lens elements with negativerefractive power is NPR. A sum of the PPR of all lens elements withpositive refractive power is ΣPPR. A sum of the NPR of all lens elementswith negative refractive powers is ΣNPR. It is beneficial to control thetotal refractive power and the total length of the optical imagecapturing system when following conditions are satisfied:0.5≤ΣPPR/|ΣNPR|≤15. Preferably, the following relation may be satisfied:1≤ΣPPR/|NPR|≤3.0.

The optical image capturing system may further include an image sensingdevice which is disposed on an image plane. Half of a diagonal of aneffective detection field of the image sensing device (imaging height orthe maximum image height of the optical image capturing system) is HOI.A distance on the optical axis from the object-side surface of the firstlens element to the image plane is HOS. The following relations aresatisfied: HOS/HOI≤50 and 0.5≤HOS/f≤150. Preferably, the followingrelations may be satisfied: 1≤HOS/HOI≤40 and 1≤HOS/f≤140. Hereby, theminiaturization of the optical image capturing system can be maintainedeffectively, so as to be carried by lightweight portable electronicdevices.

In addition, in the optical image capturing system of the disclosure,according to different requirements, at least one aperture stop may bearranged for reducing stray light and improving the imaging quality.

In the optical image capturing system of the disclosure, the aperturestop may be a front or middle aperture. The front aperture is theaperture stop between a photographed object and the first lens element.The middle aperture is the aperture stop between the first lens elementand the image plane. If the aperture stop is the front aperture, alonger distance between the exit pupil and the image plane of theoptical image capturing system can be formed, such that more opticalelements can be disposed in the optical image capturing system and theefficiency of receiving images of the image sensing device can beraised. If the aperture stop is the middle aperture, the view angle ofthe optical image capturing system can be expended, such that theoptical image capturing system has the same advantage that is owned bywide angle cameras. A distance from the aperture stop to the image planeis InS. The following relation is satisfied: 0.1≤InS/HOS≤1.1. Hereby,features of maintaining the minimization for the optical image capturingsystem and having wide-angle are available simultaneously.

In the optical image capturing system of the disclosure, a distance fromthe object-side surface of the first lens element to the image-sidesurface of the sixth lens element is InTL. A sum of central thicknessesof all lens elements with refractive power on the optical axis is ΣTP.The following relation is satisfied: 0.1≤ΣTP/InTL≤0.9. Hereby, contrastratio for the image formation in the optical image capturing system anddefect-free rate for manufacturing the lens element can be givenconsideration simultaneously, and a proper back focal length is providedto dispose other optical components in the optical image capturingsystem.

A curvature radius of the object-side surface of the first lens elementis R1. A curvature radius of the image-side surface of the first lenselement is R2. The following relation is satisfied: 0.001≤|R1/R2≤25.Hereby, the first lens element may have proper strength of the positiverefractive power, so as to avoid the longitudinal spherical aberrationto increase too fast. Preferably, the following relation may besatisfied: 0.01≤|R1/R2|<12.

A curvature radius of the object-side surface of the sixth lens elementis R11. A curvature radius of the image-side surface of the sixth lenselement is R12. The following relation is satisfied:−7<(R11−R12)/(R11+R12)<50. Hereby, the astigmatism generated by theoptical image capturing system can be corrected beneficially.

A distance between the first lens element and the second lens element onthe optical axis is IN12. The following relation is satisfied:IN12/f≤60. Hereby, the chromatic aberration of the lens elements can beimproved, such that the performance can be increased.

A distance between the fifth lens element and the sixth lens element onthe optical axis is IN56. The following relation is satisfied:IN56/f≤3.0. Hereby, the chromatic aberration of the lens elements can beimproved, such that the performance can be increased.

Central thicknesses of the first lens element and the second lenselement on the optical axis are TP1 and TP2, respectively. The followingrelation is satisfied: 0.1≤(TP1+IN12)/TP2≤10. Hereby, the sensitivityproduced by the optical image capturing system can be controlled, andthe performance can be increased.

Central thicknesses of the fifth lens element and the sixth lens elementon the optical axis are TP5 and TP6, respectively, and a distancebetween the aforementioned two lens elements on the optical axis isIN56. The following relation is satisfied: 0.1≤(TP6+IN56)/TP5≤15.Hereby, the sensitivity produced by the optical image capturing systemcan be controlled and the total height of the optical image capturingsystem can be reduced.

Central thicknesses of the second lens element, the third lens elementand the fourth lens element on the optical axis are TP2, TP3 and TP4,respectively. A distance between the second lens element and the thirdlens element on the optical axis is IN23. A distance between the thirdlens element and the fourth lens element on the optical axis is IN34. Adistance between the fourth lens element and the fifth lens element onthe optical axis is IN45. A distance on the optical axis from theobject-side surface of the first lens element to the image-side surfaceof the sixth lens element is InTL The following relation is satisfied:0.1≤TP4/(IN34+TP4+IN45)<1. Hereby, the aberration generated by theprocess of moving the incident light can be adjusted slightly layer uponlayer, and the total height of the optical image capturing system can bereduced.

In the optical image capturing system of the disclosure, a distanceperpendicular to the optical axis between a critical point C61 on theobject-side surface of the sixth lens element and the optical axis isHVT61. A distance perpendicular to the optical axis between a criticalpoint C62 on the image-side surface of the sixth lens element and theoptical axis is HVT62. A horizontal displacement distance on the opticalaxis from an axial point on the object-side surface of the sixth lenselement to the critical point C61 is SGC61. A horizontal displacementdistance on the optical axis from an axial point on the image-sidesurface of the sixth lens element to the critical point C62 is SGC62.The following relations may be satisfied: 0 mm≤HVT61≤3 mm, 0 mm<HVT62≤6mm, 0≤HVT61/HVT62, 0 mm≤|SGC61|≤0.5 mm, 0 mm<|SGC62|≤2 mm and0<|SGC62|/(|SGC62+TP6)≤0.9. Hereby, the aberration in the off-axis viewfield can be corrected.

The optical image capturing system of the disclosure satisfies thefollowing relation: 0.2≤HVT62/HOI≤0.9. Preferably, the followingrelation may be satisfied: 0.3≤HVT62/HOI≤0.8. Hereby, the aberration ofsurrounding view field can be corrected.

The optical image capturing system of the disclosure satisfies thefollowing relation: 0≤HVT62/HOS≤0.5. Preferably, the following relationmay be satisfied: 0.2≤HVT62/HOS≤0.45. Hereby, the aberration ofsurrounding view field can be corrected.

In the optical image capturing system of the disclosure, a distance inparallel with an optical axis from an inflection point on theobject-side surface of the sixth lens element which is nearest to theoptical axis to an axial point on the object-side surface of the sixthlens element is denoted by SGI611. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thesixth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the sixth lens element is denoted bySGI621. The following relations are satisfied: 0<SGI611/(SGI611+TP6)≤0.9and 0<SGI621/(SGI621+TP6)≤0.9. Preferably, the following relations maybe satisfied: 0.1≤SGI611/(SGI611+TP6)≤0.6 and0.1≤SGI621/(SGI621+TP6)≤0.6.

A distance in parallel with the optical axis from the inflection pointon the object-side surface of the sixth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the sixth lens element is denoted by SGI612. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the sixth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the sixth lenselement is denoted by SGI622. The following relations are satisfied:0<SGI612/(SGI612+TP6)≤0.9 and 0<SGI622/(SGI622+TP6)≤0.9. Preferably, thefollowing relations may be satisfied: 0.1≤SGI612/(SGI612+TP6)≤0.6 and0.1≤SGI622/(SGI622+TP6)≤0.6.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which isnearest to the optical axis and the optical axis is denoted by HIF611. Adistance perpendicular to the optical axis between an inflection pointon the image-side surface of the sixth lens element which is nearest tothe optical axis and an axial point on the image-side surface of thesixth lens element is denoted by HIF621. The following relations aresatisfied: 0.001 mm≤|HIF611|≤5 mm and 0.001 mm≤|HIF621|≤5 mm.Preferably, the following relations may be satisfied: 0.1mm≤|HIF611|≤3.5 mm and 1.5 mm≤|HIF621|≤3.5 mm.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF612. A distance perpendicular to the optical axis between an axialpoint on the image-side surface of the sixth lens element and aninflection point on the image-side surface of the sixth lens elementwhich is the second nearest to the optical axis is denoted by HIF622.The following relations are satisfied: 0.001 mm≤|HIF612|≤5 mm and 0.001mm≤|HIF622|≤5 mm. Preferably, the following relations may be satisfied:0.1 mm≤HIF622|≤3.5 mm and 0.1 mm≤|HIF612|≤3.5 mm.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thethird nearest to the optical axis and the optical axis is denoted byHIF613. A distance perpendicular to the optical axis between an axialpoint on the image-side surface of the sixth lens element and aninflection point on the image-side surface of the sixth lens elementwhich is the third nearest to the optical axis is denoted by HIF623. Thefollowing relations are satisfied: 0.001 mm≤|HIF613|≤5 mm and 0.001mm≤|HIF623|≤5 mm. Preferably, the following relations may be satisfied:0.1 mms≤|HIF623|≤3.5 mm and 0.1 mm≤|HIF613|≤3.5 mm.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thefourth nearest to the optical axis and the optical axis is denoted byHIF614. A distance perpendicular to the optical axis between an axialpoint on the image-side surface of the sixth lens element and aninflection point on the image-side surface of the sixth lens elementwhich is the fourth nearest to the optical axis is denoted by HIF624.The following relations are satisfied: 0.001 mm≤|HIF614|≤5 mm and 0.001mm≤|HIF624|≤5 mm. Preferably, the following relations may be satisfied:0.1 mm≤|HIF624|≤3.5 mm and 0.1 mm≤HIF614|3.5 mm.

In one embodiment of the optical image capturing system of the presentdisclosure, the chromatic aberration of the optical image capturingsystem can be corrected by alternatively arranging the lens elementswith large Abbe number and small Abbe number.

The above Aspheric formula is:z=ch ²/[1+[1−(k+1)c ² h ²]^(0.5) ]+A4h ⁴ +A6h ⁶ +A8h ⁸ +A10h ¹⁰ +A12h ¹²+A14h ¹⁴ +A16h ¹⁶ +A18h ¹⁸ +A20h ²⁰+  (1),where z is a position value of the position along the optical axis andat the height h which reference to the surface apex; k is the coniccoefficient, c is the reciprocal of curvature radius, and A4, A6, A8,A10, A12, A14, A16, A18, and A20 are high order aspheric coefficients.

The optical image capturing system provided by the disclosure, the lenselements may be made of glass or plastic material. If plastic materialis adopted to produce the lens elements, the cost of manufacturing willbe lowered effectively. If lens elements are made of glass, the heateffect can be controlled and the designed space arranged for therefractive power of the optical image capturing system can be increased.Besides, the object-side surface and the image-side surface of the firstthrough sixth lens elements may be aspheric, so as to obtain morecontrol variables. Comparing with the usage of traditional lens elementmade by glass, the number of lens elements used can be reduced and theaberration can be eliminated. Thus, the total height of the opticalimage capturing system can be reduced effectively.

In addition, in the optical image capturing system provided by thedisclosure, if the lens element has a convex surface, the surface of thelens element adjacent to the optical axis is convex in principle. If thelens element has a concave surface, the surface of the lens elementadjacent to the optical axis is concave in principle.

The optical image capturing system of the disclosure can be adapted tothe optical image capturing system with automatic focus if required.With the features of a good aberration correction and a high quality ofimage formation, the optical image capturing system can be used invarious application fields.

The optical image capturing system of the disclosure can include adriving module according to the actual requirements. The driving modulemay be coupled with the lens elements to enable the lens elementsproducing displacement. The driving module may be the voice coil motor(VCM) which is applied to move the lens to focus, or may be the opticalimage stabilization (OIS) which is applied to reduce the distortionfrequency owing to the vibration of the lens while shooting.

At least one of the first, second, third, fourth, fifth and sixth lenselements of the optical image capturing system of the disclosure mayfurther be designed as a light filtration element with a wavelength ofless than 500 nm according to the actual requirement. The lightfiltration element may be made by coating at least one surface of thespecific lens element characterized of the filter function, andalternatively, may be made by the lens element per se made of thematerial which is capable of filtering short wavelength.

According to the above embodiments, the specific embodiments withfigures are presented in detail as below.

The First Embodiment (Embodiment 1)

Please refer to FIG. 1A and FIG. 1B. FIG. 1A is a schematic view of theoptical image capturing system according to the first embodiment of thepresent application, FIG. 1B is longitudinal spherical aberrationcurves, astigmatic field curves, and an optical distortion curve of theoptical image capturing system in the order from left to right accordingto the first embodiment of the present application, FIG. 1C is acharacteristic diagram of modulation transfer of a visible lightaccording to the first embodiment of the present application, and FIG.1D is a characteristic diagram of modulation transfer of infrared raysaccording to the first embodiment of the present application. As shownin FIG. 1A, in order from an object side to an image side, the opticalimage capturing system includes a first lens element 110, an aperturestop 100, a second lens element 120, a third lens element 130, a fourthlens element 140, a fifth lens element 150, a sixth lens element 160, anIR-bandstop filter 180, an image plane 190, and an image sensing device192.

The first lens element 110 has negative refractive power and it is madeof plastic material. The first lens element 110 has a concaveobject-side surface 112 and a concave image-side surface 114, and bothof the object-side surface 112 and the image-side surface 114 areaspheric. The object-side surface 112 has two inflection points. Thethickness of the first lens element on the optical axis is TP1. Thethickness of the first lens element at height of ½ entrance pupildiameter (HEP) is denoted by ETP1.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the first lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefirst lens element is denoted by SGI111. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thefirst lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the first lens element is denoted bySGI121. The following relations are satisfied: SGI111=−0.0031 mm and|SGI111|/(SGI111+TP1)=0.0016.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the first lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the first lens element is denoted by SGI112. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the first lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the first lenselement is denoted by SGI122. The following relations are satisfied:SGI112=1.3178 mm and |SGI112|/(|SGI112+TP1)=0.4052.

A distance perpendicular to the optical axis from the inflection pointon the object-side surface of the first lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefirst lens element is denoted by HIF111. A distance perpendicular to theoptical axis from the inflection point on the image-side surface of thefirst lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the first lens element is denoted byHIF121. The following relations are satisfied: HIF111=0.5557 mm andHIF111/HOI=0.1111.

A distance perpendicular to the optical axis from the inflection pointon the object-side surface of the first lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the first lens element is denoted by HIF112. A distance perpendicularto the optical axis from the inflection point on the image-side surfaceof the first lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the first lenselement is denoted by HIF122. The following relations are satisfied:HIF112=5.3732 mm and HIF112/HOI=1.0746.

The second lens element 120 has positive refractive power and it is madeof plastic material. The second lens element 120 has a convexobject-side surface 122 and a convex image-side surface 124, and both ofthe object-side surface 122 and the image-side surface 124 are aspheric.The object-side surface 122 has an inflection point. The thickness ofthe second lens element on the optical axis is TP2. The thickness of thesecond lens element at height of ½ entrance pupil diameter (HEP) isdenoted by ETP2.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the second lens element which is nearest tothe optical axis to an axial point on the object-side surface of thesecond lens element is denoted by SGI211. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thesecond lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the second lens element is denoted bySGI221. The following relations are satisfied: SGI211=0.1069 mm,|SGI211|/(|SGI211|+TP2)=0.0412, SGI221=0 mm and|SGI221|/(|SGI221|+TP2)=0.

A distance perpendicular to the optical axis from the inflection pointon the object-side surface of the second lens element which is nearestto the optical axis to an axial point on the object-side surface of thesecond lens element is denoted by HIF211. A distance perpendicular tothe optical axis from the inflection point on the image-side surface ofthe second lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the second lens element is denoted byHIF221. The following relations are satisfied: HIF211=1.1264 mm,HIF211/HOI=0.2253, HIF221=0 mm and HIF221/HOI=0.

The third lens element 130 has negative refractive power and it is madeof plastic material. The third lens element 130 has a concaveobject-side surface 132 and a convex image-side surface 134, and both ofthe object-side surface 132 and the image-side surface 134 are aspheric.The object-side surface 132 and the image-side surface 134 both have aninflection point. The thickness of the third lens element on the opticalaxis is TP3. The thickness of the third lens element at height of ½entrance pupil diameter (HEP) is denoted by ETP3.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the third lens element which is nearest tothe optical axis to an axial point on the object-side surface of thethird lens element is denoted by SGI311. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thethird lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the third lens element is denoted bySGI321. The following relations are satisfied: SGI311=−0.3041 mm,|SGI311|/(SGI311|+TP3)=0.4445, SGI321=−0.1172 mm and|SGI321/(SGI321|+TP3)=0.2357.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the third lens element which isnearest to the optical axis and the optical axis is denoted by HIF311. Adistance perpendicular to the optical axis from the inflection point onthe image-side surface of the third lens element which is nearest to theoptical axis to an axial point on the image-side surface of the thirdlens element is denoted by HIF321. The following relations aresatisfied: HIF311=1.5907 mm, HIF311/HOI=0.3181, HIF321=1.3380 mm andHIF321/HOI=0.2676.

The fourth lens element 140 has positive refractive power and it is madeof plastic material. The fourth lens element 140 has a convexobject-side surface 142 and a concave image-side surface 144, and bothof the object-side surface 142 and the image-side surface 144 areaspheric. The object-side surface 142 has two inflection points and theimage-side surface 144 has an inflection point. The thickness of thefourth lens element on the optical axis is TP4. The thickness of thefourth lens element at height of ½ entrance pupil diameter (HEP) isdenoted by ETP4.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fourth lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefourth lens element is denoted by SGI411. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thefourth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the fourth lens element is denoted bySGI421. The following relations are satisfied: SGI411=0.0070 mm,|SGI411|/(|SGI411|+TP4)=0.0056, SGI421=0.0006 mm and|SGI421|/(SGI421|+TP4)=0.0005.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fourth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the fourth lens element is denoted by SGI412. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fourth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the fourth lenselement is denoted by SGI422. The following relations are satisfied:SGI412=−0.2078 mm and |SGI412|/(|SGI412|+TP4)=0.1439.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fourth lens element which isnearest to the optical axis and the optical axis is denoted by HIF411. Adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the fourth lens element which is nearest tothe optical axis and the optical axis is denoted by HIF421. Thefollowing relations are satisfied: HIF411=0.4706 mm, HIF411/HOI=0.0941,HIF421=0.1721 mm and HIF421/HOI=0.0344.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fourth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF412. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fourth lens elementwhich is the second nearest to the optical axis and the optical axis isdenoted by HIF422. The following relations are satisfied: HIF412=2.0421mm and HIF412/HOI=0.4084.

The fifth lens element 150 has positive refractive power and it is madeof plastic material. The fifth lens element 150 has a convex object-sidesurface 152 and a convex image-side surface 154, and both of theobject-side surface 152 and the image-side surface 154 are aspheric. Theobject-side surface 152 has two inflection points and the image-sidesurface 154 has an inflection point. The thickness of the fifth lenselement on the optical axis is TP5. The thickness of the fifth lenselement at height of ½ entrance pupil diameter (HEP) is denoted by ETP5.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefifth lens element is denoted by SGI511. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thefifth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the fifth lens element is denoted bySGI521. The following relations are satisfied: SGI511=0.00364 mm,|SGI511|/(SGI511|+TP5)=0.00338, SGI521=−0.63365 mm and|SGI521|/(|SGI521|+TP5)=0.37154.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the fifth lens element is denoted by SGI512. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fifth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the fifth lenselement is denoted by SGI522. The following relations are satisfied:SGI512=−0.32032 mm and SGI512/(|SGI512|+TP5)=0.23009.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is the thirdnearest to the optical axis to an axial point on the object-side surfaceof the fifth lens element is denoted by SGI513. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fifth lens element which is the third nearest to the optical axisto an axial point on the image-side surface of the fifth lens element isdenoted by SGI523. The following relations are satisfied: SGI513=0 mm,|SGI513|/(|SGI513|+TP5)=0, SGI523=0 mm and |SGI523|/(|SGI523|+TP5)=0.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is the fourthnearest to the optical axis to an axial point on the object-side surfaceof the fifth lens element is denoted by SGI514. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fifth lens element which is the fourth nearest to the opticalaxis to an axial point on the image-side surface of the fifth lenselement is denoted by SGI524. The following relations are satisfied:SGI514=0 mm, |SGI514|/(|SGI514|+TP5)=0, SGI524=0 mm and|SGI524|/(|SGI524|+TP5)=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which isnearest to the optical axis and the optical axis is denoted by HIF511. Adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the fifth lens element which is nearest tothe optical axis and the optical axis is denoted by HIF521. Thefollowing relations are satisfied: HIF511=0.28212 mm,HIF511/HOI=0.05642, HIF521=2.13850 mm and HIF521/HOI=0.42770.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF512. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fifth lens elementwhich is the second nearest to the optical axis and the optical axis isdenoted by HIF522. The following relations are satisfied: HIF512=2.51384mm and HIF512/HOI=0.50277.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which is thethird nearest to the optical axis and the optical axis is denoted byHIF513. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fifth lens elementwhich is the third nearest to the optical axis and the optical axis isdenoted by HIF523. The following relations are satisfied: HIF513=0 mm,HIF513/HOI=0, HIF523=0 mm and HIF523/HOI=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which is thefourth nearest to the optical axis and the optical axis is denoted byHIF514. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fifth lens elementwhich is the fourth nearest to the optical axis and the optical axis isdenoted by HIF524. The following relations are satisfied: HIF514=0 mm,HIF514/HOI=0, HIF524=0 mm and HIF524/HOI=0.

The sixth lens element 160 has negative refractive power and it is madeof plastic material. The sixth lens element 160 has a concaveobject-side surface 162 and a concave image-side surface 164, and theobject-side surface 162 has two inflection points and the image-sidesurface 164 has an inflection point. Hereby, the angle of incident ofeach view field on the sixth lens element can be effectively adjustedand the spherical aberration can thus be improved. The thickness of thesixth lens element on the optical axis is TP6. The thickness of thesixth lens element at height of ½ entrance pupil diameter (HEP) isdenoted by ETP6.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the sixth lens element which is nearest tothe optical axis to an axial point on the object-side surface of thesixth lens element is denoted by SGI611. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thesixth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the sixth lens element is denoted bySGI621. The following relations are satisfied: SGI611=−0.38558 mm,|SGI611|/(SGI611|+TP6)=0.27212, SGI621=0.12386 mm and|SGI621|/(|SGI621|+TP6)=0.10722.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the sixth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the sixth lens element is denoted by SGI612. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the sixth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the sixth lenselement is denoted by SGI621. The following relations are satisfied:SGI612=−0.47400 mm, |SGI612|/(|SGI612|+TP6)=0.31488, SGI622=0 mm and|SGI622|/(SGI622|+TP6)=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which isnearest to the optical axis and the optical axis is denoted by HIF611. Adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the sixth lens element which is nearest tothe optical axis and the optical axis is denoted by HIF621. Thefollowing relations are satisfied: HIF611=2.24283 mm,HIF611/HOI=0.44857, HIF621=1.07376 mm and HIF621/HOI=0.21475.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF612. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the sixth lens elementwhich is the second nearest to the optical axis and the optical axis isdenoted by HIF622. The following relations are satisfied: HIF612=2.48895mm and HIF612/HOI=−0.49779.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thethird nearest to the optical axis and the optical axis is denoted byHIF613. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the sixth lens elementwhich is the third nearest to the optical axis and the optical axis isdenoted by HIF623. The following relations are satisfied: HIF613=0 mm,HIF613/HOI=0, HIF623=0 mm and HIF623/HOI=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thefourth nearest to the optical axis and the optical axis is denoted byHIF614. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the sixth lens elementwhich is the fourth nearest to the optical axis and the optical axis isdenoted by HIF624. The following relations are satisfied: HIF614=0 mm,HIF614/HOI=0, HIF624=0 mm and HIF624/HOI=0.

In the first embodiment, a horizontal distance in parallel with theoptical axis from a coordinate point on the object-side surface of thefirst lens element at height ½ HEP to the image plane is ETL. Ahorizontal distance in parallel with the optical axis from a coordinatepoint on the object-side surface of the first lens element at height ½HEP to a coordinate point on the image-side surface of the sixth lenselement at height ½ HEP is EIN. The following relations are satisfied:ETL=19.304 mm, EIN=15.733 mm and EIN/ETL=0.815.

The first embodiment satisfies the following relations: ETP1=2.371 mm,ETP2=2.134 mm, ETP3=0.497 mm, ETP4=1.111 mm, ETP5=1.783 mm andETP6=1.404 mm. A sum of ETP1 to ETP6 described above SETP=9.300 mm.TP1=2.064 mm, TP2=2.500 mm, TP3=0.380 mm, TP4=1.186 mm, TP5=2.184 mm andTP6=1.105 mm. A sum of TP1 to TP6 described above STP=9.419 mm.SETP/STP=−0.987. SETP/EIN=0.5911.

The present embodiment particularly controls the ratio relation (ETP/TP)of the thickness (ETP) of each lens element at height of ½ entrancepupil diameter (HEP) to the thickness (TP) of the lens element to whichthe surface belongs on the optical axis in order to achieve a balancebetween manufacturability and capability of aberration correction. Thefollowing relations are satisfied: ETP1/TP1=1.149, ETP2/TP2=0.854,ETP3/TP3=1.308, ETP4/TP4=0.936, ETP5/TP5=0.817 and ETP6/TP6=1.271.

The present embodiment controls a horizontal distance between each twoadjacent lens elements at height of ½ entrance pupil diameter (HEP) toachieve a balance between the degree of miniaturization for the lengthof the optical image capturing system HOS, the manufacturability and thecapability of aberration correction. The ratio relation (ED/IN) of thehorizontal distance (ED) between the two adjacent lens elements atheight of ½ entrance pupil diameter (HEP) to the horizontal distance(IN) between the two adjacent lens elements on the optical axis isparticularly controlled. The following relations are satisfied: ahorizontal distance in parallel with the optical axis between the firstlens element and the second lens element at height of ½ entrance pupildiameter (HEP) ED12=5.285 mm; a horizontal distance in parallel with theoptical axis between the second lens element and the third lens elementat height of ½ entrance pupil diameter (HEP) ED23=0.283 mm; a horizontaldistance in parallel with the optical axis between the third lenselement and the fourth lens element at height of ½ entrance pupildiameter (HEP) ED34=0.330 mm; a horizontal distance in parallel with theoptical axis between the fourth lens element and the fifth lens elementat height of ½ entrance pupil diameter (HEP) ED45=0.348 mm; a horizontaldistance in parallel with the optical axis between the fifth lenselement and the sixth lens element at height of ½ entrance pupildiameter (HEP) ED56=0.187 mm. A sum of ED12 to ED56 described above isdenoted as SED and SED=6.433 mm.

The horizontal distance between the first lens element and the secondlens element on the optical axis IN12=5.470 mm and ED12/IN12=0.966. Thehorizontal distance between the second lens element and the third lenselement on the optical axis IN23=0.178 mm and ED23/IN23=1.590. Thehorizontal distance between the third lens element and the fourth lenselement on the optical axis IN34=0.259 mm and ED34/IN34=1.273. Thehorizontal distance between the fourth lens element and the fifth lenselement on the optical axis IN45=0.209 mm and ED45/IN45=1.664. Thehorizontal distance between the fifth lens element and the sixth lenselement on the optical axis IN56=0.034 mm and ED56/IN56=5.557. A sum ofIN12 to IN56 described above is denoted as SIN. SIN=6.150 mm.SED/SIN=1.046.

The first embodiment also satisfies the following relations:ED12/ED23=18.685, ED23/ED34=0.857, ED34/ED45=0.947, ED45/ED56=1.859,IN12/IN23=30.746, IN23/IN34=0.686, IN34/IN45=1.239 and IN45/IN56=6.207.

A horizontal distance in parallel with the optical axis from acoordinate point on the image-side surface of the sixth lens element atheight ½ HEP to the image plane EBL=3.570 mm. A horizontal distance inparallel with the optical axis from an axial point on the image-sidesurface of the sixth lens element to the image plane BL=4.032 mm. Theembodiment of the present invention may satisfy the following relation:EBL/BL=0.8854. In the present invention, a distance in parallel with theoptical axis from a coordinate point on the image-side surface of thesixth lens element at height ½ HEP to the IR-bandstop filter EIR=1.950mm. A distance in parallel with the optical axis from an axial point onthe image-side surface of the sixth lens element to the IR-bandstopfilter PIR=2.121 mm. The following relation is satisfied: EIR/PIR=0.920.

The IR-bandstop filter 180 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 160 and the image plane 190.

In the optical image capturing system of the first embodiment, a focallength of the optical image capturing system is f, an entrance pupildiameter of the optical image capturing system is HEP, and half of amaximal view angle of the optical image capturing system is HAF. Thedetailed parameters are shown as below: f=4.075 mm, f/HEP=1.4,HAF=50.001° and tan(HAF)=1.1918.

In the optical image capturing system of the first embodiment, a focallength of the first lens element 110 is f1 and a focal length of thesixth lens element 160 is f6. The following relations are satisfied:f1=−7.828 mm, |f/f1|=0.52060, f6=−4.886 and |f1|>|f6|.

In the optical image capturing system of the first embodiment, focallengths of the second lens element 120 to the fifth lens element 150 aref2, f3, f4 and f5, respectively. The following relations are satisfied:|f2|+|f3|+|f4|+|f5|=95.50815 mm, |f1|+|f6|=12.71352 mm and|f2|+|f3|+|f4|+|f5|>|f1|+|f6|.

A ratio of the focal length f of the optical image capturing system to afocal length fp of each of lens elements with positive refractive poweris PPR. A ratio of the focal length f of the optical image capturingsystem to a focal length fn of each of lens elements with negativerefractive power is NPR. In the optical image capturing system of thefirst embodiment, a sum of the PPR of all lens elements with positiverefractive power is ΣPPR=f/f1+f/f3+f/f5=1.63290. A sum of the NPR of alllens elements with negative refractive powers isΣNPR=|f/f1|+|f/f3|+|f/f6|=1.51305, ΣPPR/|ΣNPR|=1.07921. The followingrelations are also satisfied: f/f2|=0.69101, |f/f3|=0.15834,|f/f4|=0.06883, f/f5|=0.87305 and |f/f6=0.83412.

In the optical image capturing system of the first embodiment, adistance from the object-side surface 112 of the first lens element tothe image-side surface 164 of the sixth lens element is InTL. A distancefrom the object-side surface 112 of the first lens element to the imageplane 190 is HOS. A distance from an aperture 100 to an image plane 190is InS. Half of a diagonal length of an effective detection field of theimage sensing device 192 is HOI. A distance from the image-side surface164 of the sixth lens element to the image plane 190 is BFL. Thefollowing relations are satisfied: InTL+BFL=HOS, HOS=19.54120 mm,HOI=5.0 mm, HOS/HOI=3.90824, HOS/f=4.7952, InS=11.685 mm andInS/HOS=0.59794.

In the optical image capturing system of the first embodiment, a totalcentral thickness of all lens elements with refractive power on theoptical axis is ΣTP. The following relations are satisfied: ρTP=8.13899mm and ΣTP/InTL=0.52477. Hereby, contrast ratio for the image formationin the optical image capturing system and defect-free rate formanufacturing the lens element can be given considerationsimultaneously, and a proper back focal length is provided to disposeother optical components in the optical image capturing system.

In the optical image capturing system of the first embodiment, acurvature radius of the object-side surface 112 of the first lenselement is R1. A curvature radius of the image-side surface 114 of thefirst lens element is R2. The following relation is satisfied:|R1/R2|=8.99987. Hereby, the first lens element may have proper strengthof the positive refractive power, so as to avoid the longitudinalspherical aberration to increase too fast.

In the optical image capturing system of the first embodiment, acurvature radius of the object-side surface 162 of the sixth lenselement is R11. A curvature radius of the image-side surface 164 of thesixth lens element is R12. The following relation is satisfied:(R11−R12)/(R11+R12)=1.27780. Hereby, the astigmatism generated by theoptical image capturing system can be corrected beneficially.

In the optical image capturing system of the first embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=f1+f3+f5=69.770 mm andf5/(f2+f4+f5)=0.067. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the first embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=f1+f3+f6=−38.451 mm andf6/(f1+f3+f6)=0.127. Hereby, it is favorable for allocating the positiverefractive power of the sixth lens element 160 to other negative lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the first embodiment, adistance between the first lens element 110 and the second lens element120 on the optical axis is IN12. The following relations are satisfied:IN12=6.418 mm and IN12/f=1.57491. Hereby, the chromatic aberration ofthe lens elements can be improved, such that the performance can beincreased.

In the optical image capturing system of the first embodiment, adistance between the fifth lens element 150 and the sixth lens element160 on the optical axis is IN56. The following relations are satisfied:IN56=0.025 mm and IN56/f=0.00613. Hereby, the chromatic aberration ofthe lens elements can be improved, such that the performance can beincreased.

In the optical image capturing system of the first embodiment, centralthicknesses of the first lens element 110 and the second lens element120 on the optical axis are TP1 and TP2, respectively. The followingrelations are satisfied: TP1=1.934 mm, TP2=2.486 mm and(TP1+IN12)/TP2=3.36005. Hereby, the sensitivity produced by the opticalimage capturing system can be controlled, and the performance can beincreased.

In the optical image capturing system of the first embodiment, centralthicknesses of the fifth lens element 150 and the sixth lens element 160on the optical axis are TP5 and TP6, respectively, and a distancebetween the aforementioned two lens elements on the optical axis isIN56. The following relations are satisfied: TP5=1.072 mm, TP6=1.031 mmand (TP6+IN56)/TP5=0.98555. Hereby, the sensitivity produced by theoptical image capturing system can be controlled and the total height ofthe optical image capturing system can be reduced.

In the optical image capturing system of the first embodiment, adistance between the third lens element 130 and the fourth lens element140 on the optical axis is IN34. A distance between the fourth lenselement 140 and the fifth lens element 150 on the optical axis is IN45.The following relations are satisfied: IN34=0.401 mm, IN45=0.025 mm andTP4/(IN34+TP4+IN45)=0.74376. Hereby, the aberration generated by theprocess of moving the incident light can be adjusted slightly layer uponlayer, and the total height of the optical image capturing system can bereduced.

In the optical image capturing system of the first embodiment, adistance in parallel with an optical axis from a maximum effective halfdiameter position to an axial point on the object-side surface 152 ofthe fifth lens element is InRS51. A distance in parallel with an opticalaxis from a maximum effective half diameter position to an axial pointon the image-side surface 154 of the fifth lens element is InRS52. Acentral thickness of the fifth lens element 150 is TP5. The followingrelations are satisfied: InRS51=−0.34789 mm, InRS52=−0.88185 mm,|InRS51□/TP5=0.32458 and ∥InRS52□/TP5=0.82276. Hereby, it is favorablefor manufacturing and forming the lens element and for maintaining theminimization for the optical image capturing system.

In the optical image capturing system of the first embodiment, adistance perpendicular to the optical axis between a critical point C51on the object-side surface 152 of the fifth lens element and the opticalaxis is HVT51. A distance perpendicular to the optical axis between acritical point C52 on the image-side surface 154 of the fifth lenselement and the optical axis is HVT52. The following relations aresatisfied: HVT51=0.515349 mm and HVT52=0 mm.

In the optical image capturing system of the first embodiment, adistance in parallel with an optical axis from a maximum effective halfdiameter position to an axial point on the object-side surface 162 ofthe sixth lens element is InRS61. A distance in parallel with an opticalaxis from a maximum effective half diameter position to an axial pointon the image-side surface 164 of the sixth lens element is InRS62. Acentral thickness of the sixth lens element 160 is TP6. The followingrelations are satisfied: InRS61=−0.58390 mm, InRS62=0.41976 mm,∥InRS61□/TP6=0.56616 and ∥InRS62□/TP6=0.40700. Hereby, it is favorablefor manufacturing and forming the lens element and for maintaining theminimization for the optical image capturing system.

In the optical image capturing system of the first embodiment, adistance perpendicular to the optical axis between a critical point C61on the object-side surface 162 of the sixth lens element and the opticalaxis is HVT61. A distance perpendicular to the optical axis between acritical point C62 on the image-side surface 164 of the sixth lenselement and the optical axis is HVT62. The following relations aresatisfied: HVT61=0 mm and HVT62=0 mm.

In the optical image capturing system of the first embodiment, thefollowing relation is satisfied: HVT51/HOI=0.1031. Hereby, theaberration of surrounding view field can be corrected.

In the optical image capturing system of the first embodiment, thefollowing relation is satisfied: HVT51/HOS=0.02634. Hereby, theaberration of surrounding view field can be corrected.

In the optical image capturing system of the first embodiment, thesecond lens element 120, the third lens element 130 and the sixth lenselement 160 have negative refractive power. An Abbe number of the secondlens element is NA2. An Abbe number of the third lens element is NA3. AnAbbe number of the sixth lens element is NA6. The following relation issatisfied: NA6/NA2≤1. Hereby, the chromatic aberration of the opticalimage capturing system can be corrected.

In the optical image capturing system of the first embodiment, TVdistortion and optical distortion for image formation in the opticalimage capturing system are TDT and ODT, respectively. The followingrelations are satisfied: |TDT|=2.124% and |ODT|=5.076%.

In the optical image capturing system of the present embodiment,contrast transfer rates of modulation transfer with spatial frequenciesof 55 cycles/mm of a visible light at the optical axis on the imageplane, 0.3 HOI and 0.7 HOI are respectively denoted by MTFE0, MTFE3 andMTFE7. The following relations are satisfied: MTFE0 is about 0.84, MTFE3is about 0.84 and MTFE7 is about 0.75. The contrast transfer rates ofmodulation transfer with spatial frequencies of 110 cycles/mm of avisible light at the optical axis on the image plane, 0.3 HOI and 0.7HOI are respectively denoted by MTFQ0, MTFQ3 and MTFQ7. The followingrelations are satisfied: MTFQ0 is about 0.66, MTFQ3 is about 0.65 andMTFQ7 is about 0.51. The contrast transfer rates of modulation transferwith spatial frequencies of 220 cycles/mm (MTF values) at the opticalaxis on the image plane, 0.3 HOI and 0.7 HOI are respectively denoted byMTFH0, MTFH3 and MTFH7. The following relations are satisfied: MTFH0 isabout 0.17, MTFH3 is about 0.07 and MTFH7 is about 0.14.

In the optical image capturing system of the present embodiment, whenthe infrared wavelength 850 nm is applied to focus on the image plane,contrast transfer rates of modulation transfer with a spatial frequency(55 cycles/mm) (MTF values) of the image at the optical axis on theimage plane, 0.3 HOI and 0.7 HOI are respectively denoted by MTFI0,MTFI3 and MTFI7. The following relations are satisfied: MTFI0 is about0.81, MTFI3 is about 0.8 and MTFI7 is about 0.15.

Please refer to the following Table 1 and Table 2.

The detailed data of the optical image capturing system of the firstembodiment is as shown in Table 1.

TABLE 1 Data of the optical image capturing system f = 4.075 mm, f/HEP =1.4, HAF = 50.000 deg Focal Surface # Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano Plano 1 Lens 1 −40.996257041.934 Plastic 1.515 56.55 −7.828 2 4.555209289 5.923 3 Ape. stop Plano0.495 4 Lens 2 5.333427366 2.486 Plastic 1.544 55.96 5.897 5−6.781659971 0.502 6 Lens 3 −5.697794287 0.380 Plastic 1.642 22.46−25.738 7 −8.883957518 0.401 8 Lens 4 13.19225664 1.236 Plastic 1.54455.96 59.205 9 21.55681832 0.025 10 Lens 5 8.987806345 1.072 Plastic1.515 56.55 4.668 11 −3.158875374 0.025 12 Lens 6 −29.46491425 1.031Plastic 1.642 22.46 −4.886 13 3.593484273 2.412 14 IR-bandstop Plano0.200 1.517 64.13 filter 15 Plano 1.420 16 Image plane Plano Referencewavelength (d-line) = 555 nm, shield position: clear aperture (CA) ofthe first plano = 5.800 mm; clear aperture (CA) of the third plano =1.570 mm; clear aperture (CA) of the fifth plano = 1.950 mmAs for the parameters of the aspheric surfaces of the first embodiment,reference is made to Table 2.

TABLE 2 Aspheric Coefficients Surface # 1 2 4 5 6 7 8 k 4.310876E+01−4.707622E+00 2.616025E+00 2.445397E+00 5.645686E+00 −2.117147E+01−5.287220E+00 A4 7.054243E−03 1.714312E−02 −8.377541E−03 −1.789549E−02−3.379055E−03 −1.370959E−02 −2.937377E−02 A6 −5.233264E−04 −1.502232E−04−1.838068E−03 −3.657520E−03 −1.225453E−03 6.250200E−03 2.743532E−03 A83.077890E−05 −1.359611E−04 1.233332E−03 −1.131622E−03 −5.979572E−03−5.854426E−03 −2.457574E−03 A10 −1.260650E−06 2.680747E−05 −2.390895E−031.390351E−03 4.556449E−03 4.049451E−03 1.874319E−03 A12 3.319093E−08−2.017491E−06 1.998555E−03 −4.152857E−04 −1.177175E−03 −1.314592E−03−6.013661E−04 A14 −5.051600E−10 6.604615E−08 −9.734019E−04 5.487286E−051.370522E−04 2.143097E−04 8.792480E−05 A16 3.380000E−12 −1.301630E−092.478373E−04 −2.919339E−06 −5.974015E−06 −1.399894E−05 −4.770527E−06Surface # 9 10 11 12 13 k 6.200000E+01 −2.114008E+01 −7.699904E+00−6.155476E+01 −3.120467E−01 A4 −1.359965E−01 −1.263831E−01 −1.927804E−02−2.492467E−02 −3.521844E−02 A6 6.628518E−02 6.965399E−02 2.478376E−03−1.835360E−03 5.629654E−03 A8 −2.129167E−02 −2.116027E−02 1.438785E−033.201343E−03 −5.466925E−04 A10 4.396344E−03 3.819371E−03 −7.013749E−04−8.990757E−04 2.231154E−05 A12 −5.542899E−04 −4.040283E−04 1.253214E−041.245343E−04 5.548990E−07 A14 3.768879E−05 2.280473E−05 −9.943196E−06−8.788363E−06 −9.396920E−08 A16 −1.052467E−06 −5.165452E−07 2.898397E−072.494307E−07 2.728360E−09

Table 1 is the detailed structure data to the first embodiment in FIG.1A, wherein the unit of the curvature radius, the thickness, thedistance, and the focal length is millimeters (mm). Surfaces 0-16illustrate the surfaces from the object side to the image plane in theoptical image capturing system. Table 2 is the aspheric coefficients ofthe first embodiment, wherein k is the conic coefficient in the asphericsurface formula, and A1-A20 are the first to the twentieth orderaspheric surface coefficient. Besides, the tables in the followingembodiments are referenced to the schematic view and the aberrationgraphs, respectively, and definitions of parameters in the tables areequal to those in the Table 1 and the Table 2, so the repetitiousdetails will not be given here.

The Second Embodiment (Embodiment 2)

Please refer to FIG. 2A, FIG. 2B, FIGS. 2C, and 2D. FIG. 2A is aschematic view of the optical image capturing system according to thesecond embodiment of the present application, FIG. 2B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the second embodiment of the presentapplication, FIG. 2C is a characteristic diagram of modulation transferof a visible light according to the second embodiment of the presentapplication, and FIG. 2D is a characteristic diagram of modulationtransfer of infrared rays according to the second embodiment of thepresent application. As shown in FIG. 2A, in order from an object sideto an image side, the optical image capturing system includes a firstlens element 210, a second lens element 220, a third lens element 230,an aperture stop 200, a fourth lens element 240, a fifth lens element250, a sixth lens element 260, an IR-bandstop filter 280, an image plane290, and an image sensing device 292.

The first lens element 210 has negative refractive power and it is madeof glass material. The first lens element 210 has a convex object-sidesurface 212 and a concave image-side surface 214, and both of theobject-side surface 212 and the image-side surface 214 are aspheric.

The second lens element 220 has negative refractive power and it is madeof plastic material. The second lens element 220 has a concaveobject-side surface 222 and a concave image-side surface 224, and bothof the object-side surface 222 and the image-side surface 224 areaspheric.

The third lens element 230 has positive refractive power and it is madeof plastic material. The third lens element 230 has a convex object-sidesurface 232 and a convex image-side surface 234, and both of theobject-side surface 232 and the image-side surface 234 are aspheric. Theimage-side surface 234 has an inflection point.

The fourth lens element 240 has positive refractive power and it is madeof glass material. The fourth lens element 240 has a convex object-sidesurface 242 and a convex image-side surface 244, and both of theobject-side surface 242 and the image-side surface 244 are aspheric.

The fifth lens element 250 has negative refractive power and it is madeof glass material. The fifth lens element 250 has a concave object-sidesurface 252 and a convex image-side surface 254, and both of theobject-side surface 252 and the image-side surface 254 are aspheric.

The sixth lens element 260 has positive refractive power and it is madeof plastic material. The sixth lens element 260 has a convex object-sidesurface 262 and a concave image-side surface 264. The object-sidesurface 262 and the image-side surface 264 both have an inflectionpoint. Hereby, the back focal length is reduced to miniaturize the lenselement effectively. In addition, the angle of incident with incominglight from an off-axis view field can be suppressed effectively and theaberration in the off-axis view field can be corrected further.

The IR-bandstop filter 280 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 260 and the image plane 290.

In the optical image capturing system of the second embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=39.138 mm andf4/ΣPP=0.225. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the second embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−53.360 mm andf1/ΣNP=0.445. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 3 and Table 4.

The detailed data of the optical image capturing system of the secondembodiment is as shown in Table 3.

TABLE 3 Data of the optical image capturing system f = 2.735 mm, f/HEP =1.4, HAF = 100 deg Focal Surface # Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Lens 1 64.685761.925649 Glass 1.51633 64.1 −23.7643 2 10.23352 6.73208 3 Lens 2−87.4711 2.680546 Plastic 1.565 58 −7.13993 4 4.29011 3.15605 5 Lens 316.43326 2.71495 Plastic 1.65 21.4 16.3597 6 −28.8397 9.284019 7 Ape.stop Plano 0.965764 8 Lens 4 10.60194 4.246021 Glass 1.497 81.61 8.794 9−6.4705 0 10 Lens 5 −6.4705 0.3 Glass 2.00178 19.32 −22.4555 11 −9.257251.936724 12 Lens 6 7.51081 8.536279 Plastic 1.565 58 13.9846 13 84.398471 14 IR-bandstop Plano 0.85 BK_7 1.517 64.13 filter 15 Plano 0.677510 16Image plane Plano Reference wavelength (d-line) = 555 nmAs for the parameters of the aspheric surfaces of the second embodiment,reference is made to Table 4.

TABLE 4 Aspheric Coefficients Surface # 1 2 3 4 5 6 8 k 0.000000E+000.000000E+00 1.569562 −0.726312 −0.468219 −35.841629 0.000000E+00 A40.000000E+00 0.000000E+00 1.21609E−05 −2.24545E−04 1.70195E−04−2.22348E−05 0.000000E+00 A6 0.000000E+00 0.000000E+00 −7.57340E−072.35611E−06 3.18952E−06 1.33616E−06 0.000000E+00 A8 0.000000E+000.000000E+00 2.15335E−09 4.21195E−08 2.51224E−08 3.89089E−080.000000E+00 A10 0.000000E+00 0.000000E+00 −1.81730E−11 −4.71613E−091.58208E−09 7.32386E−10 0.000000E+00 Surface # 9 10 11 12 13 k0.000000E+00 0.000000E+00 0.000000E+00 −0.647875 50 A4 0.000000E+000.000000E+00 0.000000E+00 −5.26069E−05 2.50535E−03 A6 0.000000E+000.000000E+00 0.000000E+00 −1.40961E−07 −2.35354E−05 A8 0.000000E+000.000000E+00 0.000000E+00 −1.84368E−09 3.01405E−06 A10 0.000000E+000.000000E+00 0.000000E+00 −2.59433E−09 −2.23096E−07

In the second embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 3 and Table 4.

Second embodiment (Primary reference wavelength = 587.5 nm) ETP1 ETP2ETP3 ETP4 ETP5 ETP6 1.965 2.797 2.669 4.127 0.322 8.481 ETP1/TP1ETP2/TP2 ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 1.020 1.044 0.983 0.9721.075 0.993 ETL EBL EIN EIR PIR EIN/ETL 44.993  2.513 42.480  0.9921.000 0.944 SETP/EIN EIR/PIR SETP STP SETP/STP BL 0.479 0.992 20.362 20.403  0.998 2.522 ED12 ED23 ED34 ED45 ED56 EBL/BL 6.680 3.074 10.311 0.001 2.052  0.9964 SED SIN SED/SIN ED12/ED23 ED23/ED34 ED34/ED4522.118  22.076  1.002 2.173 0.298 10311.268   ED12/IN12 ED23/IN23ED34/IN34 ED45/IN45 ED56/IN56 ED45/ED56 0.992 0.974 1.006 1.000 1.059 0.00049 | f/f1 | | f/f2 | | f/f3 | | f/f4 | | f/f5 | | f/f6 |  0.11508 0.38304  0.16717  0.31099  0.12179  0.19556 Σ PPR/ TP4/(IN34 + Σ PPR ΣNPR | Σ NPR | IN12/f IN56/f TP4 + IN45)  0.67373  0.61991  1.08681 2.46157  0.70816  0.29291 | f1/f2 | | f2/f3 | (TP1 + IN12)/TP2 (TP6 +IN56)/TP5  3.32837  0.43643 3.22983 34.91000 HOS InTL HOS/HOI InS/HOSODT % TDT %  45.00000  42.47810  11.27820  0.41126 −120.35600   98.17900HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 0    0     0.00000  0.00000 0.00000  0.00000 TP2/TP3 TP3/TP4 InRS61 InRS62 | InRS61 |/TP6 | InRS62|/TP6  0.98733  0.63941  1.91828  0.65247  0.22472  0.07644 MTFE0 MTFE3MTFE7 MTFQ0 MTFQ3 MTFQ7 0.86  0.84  0.75  0.64  0.59  0.45  MTFI0 MTFI3MTFI7 0.08  0.15  0.43 

The following contents may be deduced from Table 3 and Table 4.

Related inflection point values of second embodiment (Primary referencewavelength: 555 nm) HIF321 3.9045 HIF321/HOI 0.9786 SGI321 −0.2296|SGI3216/(|SGI3216/(If) 0.0780 HIF611 5.3418 HIF611/HOI 1.3388 SGI611 1.8962 |.8962/|/(8962/HO| + TP6) 0.1818 HIF621 3.7272 HIF621/HOI 0.9341SGI621  0.5017 |SGI621//(|SGI621//(If) 0.0555

The Third Embodiment (Embodiment 3)

Please refer to FIG. 3A, FIG. 3B, FIGS. 3C, and 3D. FIG. 3A is aschematic view of the optical image capturing system according to thethird embodiment of the present application, FIG. 3B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the third embodiment of the presentapplication, FIG. 3C is a characteristic diagram of modulation transferof a visible light according to the third embodiment of the presentapplication, and FIG. 3D is a characteristic diagram of modulationtransfer of infrared rays according to the third embodiment of thepresent application. As shown in FIG. 3A, in order from an object sideto an image side, the optical image capturing system includes a firstlens element 310, a second lens element 320, a third lens element 330,an aperture stop 300, a fourth lens element 340, a fifth lens element350, a sixth lens element 360, an IR-bandstop filter 380, an image plane390, and an image sensing device 392.

The first lens element 310 has negative refractive power and it is madeof glass material. The first lens element 310 has a convex object-sidesurface 312 and a concave image-side surface 314, and both of theobject-side surface 312 and the image-side surface 314 are aspheric.

The second lens element 320 has negative refractive power and it is madeof glass material. The second lens element 320 has a convex object-sidesurface 322 and a concave image-side surface 324, and both of theobject-side surface 322 and the image-side surface 324 are aspheric

The third lens element 330 has negative refractive power and it is madeof plastic material. The third lens element 330 has a concaveobject-side surface 332 and a concave image-side surface 334, and bothof the object-side surface 332 and the image-side surface 334 areaspheric.

The fourth lens element 340 has positive refractive power and it is madeof glass material. The fourth lens element 340 has a convex object-sidesurface 342 and a convex image-side surface 344, and both of theobject-side surface 342 and the image-side surface 344 are aspheric.

The fifth lens element 350 has positive refractive power and it is madeof plastic material. The fifth lens element 350 has a convex object-sidesurface 352 and a convex image-side surface 354, and both of theobject-side surface 352 and the image-side surface 354 are aspheric. Theobject-side surface 352 has an inflection point.

The sixth lens element 360 has negative refractive power and it is madeof plastic material. The sixth lens element 360 has a concaveobject-side surface 362 and a concave image-side surface 364. Theobject-side surface 362 and the mage-side surface 364 both have aninflection point. Hereby, the back focal length is reduced tominiaturize the lens element effectively. In addition, the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 380 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 360 and the image plane 390.

In the optical image capturing system of the third embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=17.313 mm andf4/ΣPP=0.529. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the third embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−103.166 mm andf1/ΣNP=0.113. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 5 and Table 6.

The detailed data of the optical image capturing system of the thirdembodiment is as shown in Table 5.

TABLE 5 Data of the optical image capturing system f = 3.40816 mm; f/HEP= 1.6; HAF = 90.05 deg Focal Surface# Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano At infinity 1 Lens 166.77321 2.232047 Glass 1.497 81.61 −11.6113 2 5.26359 2.477945 3 Lens 218.41423 0.853001 Glass 1.51633 64.1 −14.5 4 5.2492 1.837199 5 Lens 3−104.47 8.795838 Plastic 1.65 21.4 −60.8831 6 66.72218 0.058462 7 Ape.Stop Plano 0.052067 8 Lens 4 9.30752 2.404947 Glass 1.497 81.61 9.153479 −8.17008 1.512149 10 Lens 5 5.82652 3.07992 Plastic 1.565 58 8.1590311 −18.1274 0.554318 12 Lens 6 −11.2323 0.622305 Plastic 1.65 21.4−16.1715 13 192.2671 1 14 IR-bandstop Plano 0.85 BK_7 1.517 64.13 filter15 Plano 3.662281 16 Image plane Plano Reference wavelength (d-line) =555 nmAs for the parameters of the aspheric surfaces of the third embodiment,reference is made to Table 6.

TABLE 6 Aspheric Coefficients Surface # 1 2 3 4 5 6 8 k 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 −8.95217 −28.897867 0.000000E+00A4 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 −1.06346E−03−2.63319E−04 0.000000E+00 A6 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 −5.48917E−05 2.70072E−05 0.000000E+00 A8 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 1.16564E−06 9.21640E−080.000000E+00 A10 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00−1.24968E−07 9.00631E−09 0.000000E+00 Surface # 9 10 11 12 13 k0.000000E+00 −4.590841 2.805394 −5.647697 19.519685 A4 0.000000E+001.83242E−03 −2.81557E−03 −1.07933E−03 3.13280E−03 A6 0.000000E+00−1.01493E−04 9.02524E−05 5.02717E−05 −4.58211E−05 A8 0.000000E+001.29923E−08 1.79522E−06 9.97081E−06 2.44375E−06 A10 0.000000E+00−3.13883E−08 −1.05969E−07 −3.60233E−07 −1.68579E−07

The presentation of the aspheric surface formula in the third embodimentis similar to that in the first embodiment. Besides, the definitions ofparameters in following tables are equal to those in the firstembodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 5 and Table 6.

Third embodiment (Primary reference wavelength: 555 nm) ETP1 ETP2 ETP3ETP4 ETP5 ETP6 2.332 0.931 8.811 2.274 2.948 0.681 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 1.045 1.092 1.002 0.946 0.957 1.094ETL EBL EIN EIR PIR EIN/ETL 29.984  5.505 24.479  0.993 1.000 0.816SETP/EIN EIR/PIR SETP STP SETP/STP BL 0.734 0.993 17.978  17.988  0.9995.512 ED12 ED23 ED34 ED45 ED56 EBL/BL 2.400 1.721 0.163 1.679 0.538 0.9987 SED SIN SED/SIN ED12/ED23 ED23/ED34 ED34/ED45 6.501 6.492 1.0011.394 10.528  0.097 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45 ED56/IN56ED45/ED56 0.969 0.937 1.479 1.110 0.970 3.121 | f/f1 | | f/f2 | | f/f3 || f/f4 | | f/f5 | | f/f6 |  0.29352  0.23505  0.05598  0.37234  0.41772 0.21075 Σ PPR/ TP4/(IN34 + Σ PPR Σ NPR | Σ NPR | IN12/f IN56/f TP4 +IN45)  0.42831  0.79530  0.53856  0.72706  0.16264  0.59711 | f1/f2 | |f2/f3 | (TP1 + IN12)/TP2 (TP6 + IN56)/TP5  0.80078  0.23816 5.521680.38203 HOS InTL HOS/HOI InS/HOS ODT % TDT %  29.99240  24.48020 7.52632  0.45805 −97.17900  75.37130 HVT51 HVT52 HVT61 HVT62 HVT62/HOIHVT62/HOS 0    0     3.66864  0.00000  0.00000  0.00000 TP2/TP3 TP3/TP4InRS61 InRS62 | InRS61 |/TP6 | InRS62 |/TP6  0.09698  3.65739  −0.40351 0.59825  0.64841  0.96135 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.85 0.88  0.85  0.62  0.72  0.63  MTFI0 MTFI3 MTFI7 0.57  0.65  0.28 

The following contents may be deduced from Table 5 and Table 6.

Related inflection point values of third embodiment (Primary referencewavelength: 555 nm) HIF511 2.9861 HIF511/HOI 0.7493 SGI511  0.7113|.7113/|/(7113/HO| + TP5) 0.1876 HIF611 2.5020 HIF611/HOI 0.6279 SGI611−0.2823 |0.2823/(.2823HO| + TP6) #REF! HIF621 3.8179 HIF621/HOI 0.9581SGI621  0.5611 |SGI621//(|SGI621//(It) #REF!

The Fourth Embodiment (Embodiment 4)

Please refer to FIG. 4A, FIG. 4B, FIGS. 4C, and 4D. FIG. 4A is aschematic view of the optical image capturing system according to thefourth embodiment of the present application, FIG. 4B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the fourth embodiment of the presentapplication, FIG. 4C is a characteristic diagram of modulation transferof a visible light according to the fourth embodiment of the presentapplication, and FIG. 4D is a characteristic diagram of modulationtransfer of infrared rays according to the fourth embodiment of thepresent application. As shown in FIG. 4A, in order from an object sideto an image side, the optical image capturing system includes a firstlens element 410, a second lens element 420, a third lens element 430,an aperture stop 400, a fourth lens element 440, a fifth lens element450, a sixth lens element 460, an IR-bandstop filter 480, an image plane490, and an image sensing device 492.

The first lens element 410 has negative refractive power and it is madeof glass material. The first lens element 410 has a convex object-sidesurface 412 and a concave image-side surface 414, and both of theobject-side surface 412 and the image-side surface 414 are aspheric.

The second lens element 420 has negative refractive power and it is madeof plastic material. The second lens element 420 has a convexobject-side surface 422 and a concave image-side surface 424, and bothof the object-side surface 422 and the image-side surface 424 areaspheric. The object-side surface 422 has an inflection point.

The third lens element 430 has positive refractive power and it is madeof glass material. The third lens element 430 has a convex object-sidesurface 432 and a concave image-side surface 434, and both of theobject-side surface 432 and the image-side surface 434 are aspheric.

The fourth lens element 440 has positive refractive power and it is madeof plastic material. The fourth lens element 440 has a convexobject-side surface 442 and a convex image-side surface 444, and both ofthe object-side surface 442 and the image-side surface 444 are aspheric.The object-side surface 442 has an inflection point.

The fifth lens element 450 has positive refractive power and it is madeof glass material. The fifth lens element 450 has a convex object-sidesurface 452 and a convex image-side surface 454, and both of theobject-side surface 452 and the image-side surface 454 are aspheric.

The sixth lens element 460 has positive refractive power and it is madeof plastic material. The sixth lens element 460 has a convex object-sidesurface 462 and a concave image-side surface 464. The object-sidesurface 462 has an inflection point and the image-side surface 464 hastwo inflection points. Hereby, the back focal length is reduced tominiaturize the lens element effectively. In addition, the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 480 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 460 and the image plane 490.

In the optical image capturing system of the fourth embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=111.293 mm andf4/ΣPP=0.065. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the fourth embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−22.659 mm andf1/ΣNP=0.672. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 7 and Table 8.

The detailed data of the optical image capturing system of the fourthembodiment is as shown in Table 7.

TABLE 7 Data of the optical image capturing system f = 2.460 mm; f/HEP =1.6; HAF = 70.00 deg Focal Surface# Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Lens 1 561.88071.781331 Glass 1.497 81.61 −15.2173 2 7.47121 1.351266 3 Lens 2 11.115632.699904 Plastic 1.565 54.5 −7.4418 4 2.78934 3.099904 5 Lens 3 13.822239.974673 Glass 2.00272 19.32 65.9907 6 11.10334 0.28217 7 Ape. StopPlano 0.05 8 Lens 4 6.91461 1.422216 Plastic 1.565 58 7.24079 9 −9.344980.05 10 Lens 5 5.71659 2.221029 Glass 1.497 81.61 7.96895 11 −11.31032.649626 12 Lens 6 13.86023 3.038935 Plastic 1.65 21.4 30.0923 1342.57531 0.5 14 IR-bandstop Plano 0.85 BK_7 1.517 64.13 filter 15 Plano0.028959 16 Image plane Plano Reference wavelength (d-line) = 555 nmAs for the parameters of the aspheric surfaces of the fourth embodiment,reference is made to Table 8l

TABLE 8 Aspheric Coefficients Surface # 3 4 5 6 8 9 10 k −2.895753E+00−5.305419E−01 0.000000E+00 0.000000E+00 1.287252E+00 −7.238133E−02−1.102549E+00 A4 −6.872493E−04 −5.196963E−04 0.000000E+00 0.000000E+004.118629E−04 8.346616E−05 −3.694356E−04 A6 −5.713381E−05 −9.126514E−050.000000E+00 0.000000E+00 −1.136292E−05 3.769059E−06 −6.297694E−05 A8−4.922138E−07 7.401893E−06 0.000000E+00 0.000000E+00 −2.276806E−06−9.982125E−07 2.259523E−06 A10 4.379280E−08 −1.324272E−06 0.000000E+000.000000E+00 9.598033E−08 7.401288E−08 −4.631574E−07 Surface # 11 12 13k −3.507269E−02 8.157804E−02 −1.679229E+01 A4 −3.892551E−04 2.276216E−031.527674E−03 A6 4.799095E−05 1.211605E−04 6.710888E−05 A8 8.167494E−06−4.236754E−07 −4.237391E−06 A10 −3.644669E−07 3.715526E−07 4.259586E−08

The presentation of the aspheric surface formula in the fourthembodiment is similar to that in the first embodiment. Besides thedefinitions of parameters in following tables are equal to those in thefirst embodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 7 and Table 8.

fourth embodiment (Primary reference wavelength: 587.5 nm) ETP1 ETP2ETP3 ETP4 ETP5 ETP6 1.820 2.780 9.980 1.348 2.143 3.027 ETP1/TP1ETP2/TP2 ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 1.022 1.030 1.001 0.9480.965 0.996 ETL EBL EIN EIR PIR EIN/ETL 29.999  1.372 28.627  0.4930.500 0.954 SETP/EIN EIR/PIR SETP STP SETP/STP BL 0.737 0.987 21.098 21.138  0.998 1.379 ED12 ED23 ED34 ED45 ED56 EBL/BL 1.338 3.014 0.3480.134 2.695  0.9949 SED SIN SED/SIN ED12/ED23 ED23/ED34 ED34/ED45 7.5297.483 1.006 0.444 8.665 2.602 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45ED56/IN56 ED45/ED56 0.991 0.972 1.047 2.674 1.017 0.050 | f/f1 | | f/f2| | f/f3 | | f/f4 | | f/f5 | | f/f6 |  0.16168  0.33062  0.03728 0.33980  0.0875  0.08176 Σ PPR/ TP4/(IN34 + Σ PPR Σ NPR | Σ NPR |IN12/f IN56/f TP4 + IN45)  0.91528  0.49230  1.85917  0.54921  1.07691 0.78820 | f1/f2 | | f2/f3 | (TP1 + IN12)/TP2 (TP6 + IN56)/TP5  2.04484 0.11277 1.16027 2.56123 HOS InTL HOS/HOI InS/HOS ODT % TDT %  30.00000 28.62110  7.50000  0.36036 −40.79820  32.74790 HVT51 HVT52 HVT61 HVT62HVT62/HOI HVT62/HOS 0    0     1.53515  1.74017  0.43504  0.05801TP2/TP3 TP3/TP4 InRS61 InRS62 | InRS61 |/TP6 | InRS62 |/TP6  0.27068 7.01345  −0.36379  −0.43648  0.11971  0.14363 MTFE0 MTFE3 MTFE7 MTFQ0MTFQ3 MTFQ7 0.86  0.79  0.68  0.67  0.46  0.39  MTFI0 MTFI3 MTFI7 0.75 0.68  0.26 

The following contents may be deduced from Table 7 and Table 8.

Related inflection point values of second embodiment (Primary referencewavelength: 555 nm) HIF211 5.7875 HIF211/HOI 1.4469 SGI211  2.0360|.0360/|/(0360/HO| + TP2) 0.4299 HIF411 2.1575 HIF411/HOI 0.5394 SGI411 0.3051 |.3051/|/(3051/HO| + TP4) 0.1766 HIF611 0.9293 HIF611/HOI 0.2323SGI611  0.0263 |.0263/|/(0263/HO| + TP6) 0.0086 HIF621 1.1285 HIF621/HOI0.2821 SGI621  0.0134 |SGI621//(|SGI621//(If) 0.0044 HIF622 3.5566HIF622/HOI 0.8891 SGI622 −0.3795 |SGI6225/(|SGI6225/(If) 0.1110

The Fifth Embodiment (Embodiment 5)

Please refer to FIG. 5A, FIG. 5B, FIGS. 5C, and 5D. FIG. 5A is aschematic view of the optical image capturing system according to thefifths embodiment of the present application, FIG. 5B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the fifth embodiment of the presentapplication, FIG. 5C is a characteristic diagram of modulation transferof a visible light according to the fifth embodiment of the presentapplication and FIG. 5D is a characteristic diagram of modulationtransfer of infrared rays according to the fifth embodiment of thepresent application. As shown in FIG. 5A, in order from an object sideto an image side, the optical image capturing system includes a firstlens element 510, a second lens element 520, a third lens element 530,an aperture stop 500, a fourth lens element 540, a fifth lens element550, a sixth lens element 560, an IR-bandstop filter 580, an image plane590, and an Image sensing device 592.

The first lens element 510 has negative refractive power and it is madeof glass material. The first lens element 510 has a convex object-sidesurface 512 and a concave image-side surface 514, and both of theobject-side surface 512 and the image-side surface 514 are aspheric.

The second lens element 520 has negative refractive power and it is madeof plastic material. The second lens element 520 has a convexobject-side surface 522 and a concave image-side surface 524, and bothof the object-side surface 522 and the image-side surface 524 areaspheric. The object-side surface 522 has an inflection point.

The third lens element 530 has positive refractive power and it is madeof glass material. The third lens element 530 has a convex object-sidesurface 532 and a concave image-side surface 534, and both of theobject-side surface 532 and the image-side surface 534 are aspheric.

The fourth lens element 540 has positive refractive power and it is madeof plastic material. The fourth lens element 540 has a convexobject-side surface 542 and a convex image-side surface 544, and both ofthe object-side surface 542 and the image-side surface 544 are aspheric.The object-side surface 542 has an inflection point.

The fifth lens element 550 has negative refractive power and it is madeof glass material. The fifth lens element 550 has a concave object-sidesurface 552 and a convex image-side surface 554, and both of theobject-side surface 552 and the image-side surface 554 are aspheric.

The sixth lens element 560 has positive refractive power and it is madeof plastic material. The sixth lens element 560 has a convex object-sidesurface 562 and a concave image-side surface 564. The image-side surface564 has an inflection point. Hereby, the back focal length is reduced tominiaturize the lens element effectively. In addition, the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 580 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 560 and the image plane 590.

In the optical image capturing system of the fifth embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=24.210 mm andf4/ΣPP=0.274. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the fifth embodiment, sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−32.690 mm andf1/ΣNP=0.512. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 9 and Table 10.

The detailed data of the optical image capturing system of the fifthembodiment is as shown in Table 9.

TABLE 9 Data of the optical image capturing system f = 2.731 mm; f/HEP =2.0; HAF = 90.05 deg Focal Surface# Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Lens 1 158.71251.948162 Glass 1.497 81.61 −16.7371 2 7.8886 2.278267 3 Lens 2 11.976182.45277 Plastic 1.565 58 −8.8418 4 3.27125 7.678807 5 Lens 3 6.830551.143514 Glass 1.85026 32.2 9.07105 6 52.83123 2.168908 7 Ape. StopPlano 0.613869 8 Lens 4 40.58743 2.815528 Plastic 1.565 58 6.62896 9−4.03654 0.05 10 Lens 5 −3.52936 0.42814 Glass 2.00272 19.32 −7.11082 11−7.34922 1.081539 12 Lens 6 4.14836 4.775589 Plastic 1.565 58 8.51001 1317.29949 1 14 IR-bandstop Plano 0.85 BK_7 1.517 64.13 filter 15 Plano0.713831 16 Image plane Plano Reference wavelength (d-line) = 555 nmAs for the parameters of the aspheric surfaces of the filth embodiment,reference is made to Table 10.

TABLE 10 Aspheric Coefficients Surface # 1 2 3 4 5 6 8 k 0.000000E+000.000000E+00 0.927525 −0.604339 0.000000E+00 0.000000E+00 −32.086794 A40.000000E+00 0.000000E+00 2.13966E−04 4.54505E−05 0.000000E+000.000000E+00 −2.71924E−03 A6 0.000000E+00 0.000000E+00 −2.05886E−061.85939E−05 0.000000E+00 0.000000E+00 −3.35570E−04 A8 0.000000E+000.000000E+00 −5.15866E−08 −9.01497E−07 0.000000E+00 0.000000E+001.48631E−04 A10 0.000000E+00 0.000000E+00 −1.06716E−09 −1.67996E−070.000000E+00 0.000000E+00 −4.21909E−05 Surface # 9 10 11 12 13 k0.900289 0.000000E+00 0.000000E+00 −5.698577 7.307759 A4 −1.01800E−020.000000E+00 0.000000E+00 1.13955E−03 8.80338E−04 A6 1.40865E−030.000000E+00 0.000000E+00 −2.52170E−05 −4.77208E−05 A8 −1.21578E−040.000000E+00 0.000000E+00 1.81875E−06 −2.00898E−06 A10 6.56126E−060.000000E+00 0.000000E+00 −3.27995E−08 7.62651E−08

The presentation of the aspheric surface formula in the fifth embodimentis similar to that in the first embodiment. Besides the definitions ofparameters in following tables are equal to those in the firstembodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 9 and Table 10.

Fifth embodiment (Primary reference wavelength: 587.5 nm) ETP1 ETP2 ETP3ETP4 ETP5 ETP6 1.976 2.505 1.114 2.750 0.463 4.735 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 1.014 1.021 0.974 0.977 1.081 0.991ETL EBL EIN EIR PIR EIN/ETL 29.997  2.550 27.447  0.986 1.000 0.915SETP/EIN EIR/PIR SETP STP SETP/STP BL 0.493 0.986 13.542  13.564  0.9982.564 ED12 ED23 ED34 ED45 ED56 EBL/BL 2.268 7.641 2.783 0.044 1.168 0.9945 SED SIN SED/SIN ED12/ED23 ED23/ED34 ED34/ED45 13.905  13.871 1.002 0.297 2.745 63.326  ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45ED56/IN56 ED45/ED56 0.996 0.995 1.000 0.879 1.080 0.038 | f/f1 | | f/f2| | f/f3 | | f/f4 | | f/f5 | | f/f6 |  0.16317  0.30886  0.30106 0.41197  0.38405  0.32091 Σ PPR/ TP4/(IN34 + Σ PPR Σ NPR | Σ NPR |IN12/f IN56/f TP4 + IN45)  1.03393  0.85608  1.20775  0.83425  0.39604 0.49847 | f1/f2 | | f2/f3 | (TP1 + IN12)/TP2 (TP6 + IN56)/TP5  1.89295 0.97473 1.72313 13.68041 HOS InTL HOS/HOI InS/HOS ODT % TDT %  29.99890 27.43510  7.49973  0.41097 −100.15900   84.30610 HVT51 HVT52 HVT61HVT62 HVT62/HOI HVT62/HOS 0    0     0.00000  0.00000  0.00000  0.00000TP2/TP3 TP3/TP4 InRS61 InRS62 | InRS61 |/TP6 | InRS62 |/TP6  2.14495 0.40614  0.95926  0.40349  0.20087  0.08449 MTFE0 MTFE3 MTFE7 MTFQ0MTFQ3 MTFQ7 0.86  0.85  0.74  0.67  0.65  0.48  MTFI0 MTFI3 MTFI7 0.88 0.85  0.54 

The following contents may be deduced from Table 9 and Table 10.

Related inflection point values of fifth embodiment (Primary referencewavelength: 555 nm) HIF211 5.7489 HIF211/HOI 1.4372 SGI211 1.6367|SGI211|/(|SGI211| + TP2) 0.4002 HIF411 0.8115 HIF411/HOI 0.2029 SGI4110.0068 |SGI411|/(|SGI411| + TP4) 0.0024 HIF621 3.2659 HIF621/HOI 0.8165SGI621 0.3620 |SGI621|/(|SGI621| + TP6) 0.0705

The Sixth Embodiment (Embodiment 6)

Please refer to FIG. 6A, FIG. 6B, FIGS. 6C, and 6D. FIG. 6A is aschematic view of the optical image capturing system according to thesixth Embodiment of the present application, FIG. 6B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the sixth Embodiment of the presentapplication, FIG. 6C is a characteristic diagram of modulation transferof a visible light according to the sixth embodiment of the presentapplication and FIG. 6D is a characteristic diagram of modulationtransfer of infrared rays according to the sixth embodiment of thepresent application. As shown in FIG. 6A, in order from an object sideto an image side, the optical image capturing system includes a firstlens element 610, a second lens element 620, a third lens element 630,an aperture stop 600, a fourth lens element 640, a fifth lens element650, a sixth lens element 660, an IR-bandstop filter 680, an image plane690, and an image sensing device 692.

The first lens element 610 has negative refractive power and it is madeof glass material. The first lens element 610 has a convex object-sidesurface 612 and a concave image-side surface 614, and both of theobject-side surface 612 and the image-side surface 614 are aspheric.

The second lens element 620 has negative refractive power and it is madeof plastic material. The second lens element 620 has a convexobject-side surface 622 and a concave image-side surface 624, and bothof the object-side surface 622 and the image-side surface 624 areaspheric and have an inflection point.

The third lens element 630 has positive refractive power and it is madeof glass material. The third lens element 630 has a convex object-sidesurface 632 and a concave image-side surface 634, and both of theobject-side surface 632 and the image-side surface 634 are aspheric.

The fourth lens element 640 has positive refractive power and it is madeof plastic material. The fourth lens element 640 has a convexobject-side surface 642 and a convex image-side surface 644, and both ofthe object-side surface 642 and the image-side surface 644 are aspheric.The object-side surface 642 has an inflection point.

The fifth lens element 650 has positive refractive power and it is madeof glass material. The fifth lens element 650 has a convex object-sidesurface 652 and a convex image-side surface 654, and both of theobject-side surface 652 and the image-side surface 654 are aspheric.

The sixth lens element 660 has positive refractive power and it is madeof plastic material. The sixth lens element 660 has a concaveobject-side surface 662 and a convex image-side surface 664. Hereby, theback focal length is reduced to miniaturize the lens elementeffectively. In addition, the angle of incident with incoming light froman off-axis view field can be suppressed effectively and the aberrationin the off-axis view field can be corrected further.

The IR-bandstop filter 680 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 660 and the image plane 690.

In the optical image capturing system of the sixth Embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=66.900 mm andf4/ΣPP=0.089. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the sixth Embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=−28.048 mm andf1/ΣNP=0.787. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 11 and Table 12.

The detailed data of the optical image capturing system of the sixthEmbodiment is as shown in Table 11.

TABLE 11 Data of the optical image capturing system f = 2.444 mm; f/HEP= 2.0; HAF = 70.000 deg Focal Surface# Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano At infinity 1 Lens 164.73725 1.769099 Glass 1.497 81.61 −22.0634 2 9.30979 1.213527 3 Lens 211.28133 2.000545 Plastic 1.565 58 −5.98497 4 2.44067 3.539669 5 Lens 38.99034 8.952897 Glass 2.00272 19.32 39.015 6 5.81026 0.853199 7 Ape.Stop Plano 0.05 8 Lens 4 7.48448 2.086861 Plastic 1.565 58 5.98404 9−5.57661 0.412171 10 Lens 5 5.29685 1.962138 Glass 1.497 81.61 7.7628711 −12.5586 2.295313 12 Lens 6 −45.7341 3.48915 Plastic 1.65 21.414.1376 13 −7.93795 0.5 14 IR-bandstop Plano 0.85 BK_7 1.517 64.13filter 15 Plano 0.025399 16 Image plane Plano Reference wavelength(d-line) = 555 nmAs for the parameters of the aspheric surfaces of the sixth Embodiment,reference is made to Table 12.

TABLE 12 Aspheric Coefficients Surface # 3 4 5 6 8 9 10 k −0.878141−0.744684 0.000000E+00 0.000000E+00 11.901861 −1.175121 0.000000E+00 A44.60534E−04 8.63870E−04 0.000000E+00 0.000000E+00 −6.39244E−03−2.06820E−03 0.000000E+00 A6 −7.14692E−06 −1.14380E−05 0.000000E+000.000000E+00 −6.53140E−04 −1.82876E−04 0.000000E+00 A8 −7.24993E−082.81209E−06 0.000000E+00 0.000000E+00 −1.88084E−05 6.72122E−060.000000E+00 A10 4.04555E−10 −5.15683E−07 0.000000E+00 0.000000E+00−4.19272E−05 −4.91052E−06 0.000000E+00 Surface # 11 12 13 k 0.000000E+0050 −15.401579 A4 0.000000E+00 −6.20415E−03 −5.73797E−04 A6 0.000000E+00−4.61478E−04 −8.18676E−05 A8 0.000000E+00 3.45645E−06 −4.06629E−07 A100.000000E+00 −4.32860E−06 5.29741E−08

In the sixth Embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 11 and Table 12.

Sixth embodiment (Primary reference wavelength: 555 nm) ETP1 ETP2 ETP3ETP4 ETP5 ETP6 1.786 2.061 8.964 2.029 1.912 3.471 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 1.010 1.030 1.001 0.972 0.974 0.995ETL EBL EIN EIR PIR EIN/ETL 29.997  1.398 28.599  0.523 0.500 0.953SETP/EIN EIR/PIR SETP STP SETP/STP BL 0.707 1.046 20.223  20.261  0.9981.375 ED12 ED23 ED34 ED45 ED56 EBL/BL 1.210 3.484 0.896 0.481 2.305 1.0167 SED SIN SED/SIN ED12/ED23 ED23/ED34 ED34/ED45 8.376 8.364 1.0010.347 3.890 1.861 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45 ED56/IN56ED45/ED56 0.997 0.984 0.992 1.168 1.004 0.209 | f/f1 | | f/f2 | | f/f3 || f/f4 | | f/f5 | | f/f6 |  0.11077  0.40835  0.06264  0.40841  0.31483 0.17287 Σ PPR/ TP4/(IN34 + Σ PPR Σ NPR | Σ NPR | IN12/f IN56/f TP4 +IN45  1.10679  0.51912  2.13204  0.49654  0.93917  0.61338 | f1/f2 | |f2/f3 | (TP1 + IN12)/TP2 (TP6 + IN56)/TP5  3.68647  0.15340 1.490912.94804 HOS InTL HOS/HOI InS/HOS ODT % TDT %  29.99990  28.62460 7.49998  0.38903 −40.39990  38.32870 HVT51 HVT52 HVT61 HVT62 HVT62/HOIHVT62/HOS 0    0     0.00000  0.00000  0.00000  0.00000 TP2/TP3 TP3/TP4InRS61 InRS62 | InRS61 |/TP6 | InRS62 |/TP6  0.22345  4.29013  −0.62941 −0.89702  0.18039  0.25709 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.86 0.78  0.7  0.7  0.52  0.4  MTFI0 MTFI3 MTFI7 0.86  0.78  0.65 

The following contents may be deduced from Table 11 and Table 12.

Related inflection point values of sixth embodiment (Primary referencewavelength: 555 nm) HIF211 5.3794 HIF211/HOI 1.3448 SGI211 1.4614|.4614/|/(4614/HO| + TP2) 0.4221 HIF221 4.0056 HIF221/HOI 1.0014 SGI2214.0303 |SGI221//(|SGI221//(It) 0.6683

The Seventh Embodiment (Embodiment 7)

Please refer to FIG. 7A and FIG. 7B, FIGS. 7C, and 7D. FIG. 7A is aschematic view of the optical image capturing system according to theseventh Embodiment of the present application, FIG. 7B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the seventh Embodiment of the presentapplication, FIG. 7C is a characteristic diagram of modulation transferof a visible light according to the seventh embodiment of the presentapplication and FIG. 7D is a characteristic diagram of modulationtransfer of infrared rays according to the seventh embodiment of thepresent application. As shown in FIG. 7A, in order from an object sideto an image side, the optical image capturing system includes a firstlens element 710, a second lens element 720, an aperture stop 700, athird lens element 730, a fourth lens element 740, a fifth lens element750, a sixth lens element 760, an IR-bandstop filter 780, an image plane790, and an image sensing device 792.

The first lens element 710 has negative refractive power and it is madeof glass material. The first lens element 710 has a convex object-sidesurface 712 and a concave image-side surface 714, and both of theobject-side surface 712 and the image-side surface 714 are aspheric.

The second lens element 720 has positive refractive power and it is madeof plastic material. The second lens element 720 has a convexobject-side surface 722 and a concave image-side surface 724, and bothof the object-side surface 722 and the image-side surface 724 areaspheric.

The third lens element 730 has positive refractive power and it is madeof glass material. The third lens element 730 has a convex object-sidesurface 732 and a convex image-side surface 734, and both of theobject-side surface 732 and the image-side surface 734 are aspheric.

The fourth lens element 740 has negative refractive power and it is madeof plastic material. The fourth lens element 740 has a concaveobject-side surface 742 and a convex image-side surface 744, and both ofthe object-side surface 742 and the image-side surface 744 are aspheric.The object-side surface 742 has an inflection point.

The fifth lens element 750 has positive refractive power and it is madeof plastic material. The fifth lens element 750 has a concaveobject-side surface 752 and a convex image-side surface 754, and both ofthe object-side surface 752 and the image-side surface 754 are aspheric.The image-side surface 754 has an inflection point.

The sixth lens element 760 has positive refractive power and it is madeof plastic material. The sixth lens element 760 has a concaveobject-side surface 762 and a convex image-side surface 764. Hereby, theback focal length is reduced to miniaturize the lens elementeffectively. In addition, the angle of incident with incoming light froman off-axis view field can be suppressed effectively and the aberrationin the off-axis view field can be corrected further.

The IR-bandstop filter 780 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 760 and the image plane 790.

In the optical image capturing system of the seventh Embodiment, a sumof focal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=66.333 mm andf2/ΣPP=0.540. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the seventh Embodiment, a sumof focal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=−7.968 mm andf1/ΣNP=0.627. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 13 and Table 14.

The detailed data of the optical image capturing system of the seventhEmbodiment is as shown in Table 13.

TABLE 13 Data of the optical image capturing system f = 3.734 mm; f/HEP= 2.8; HAF = 60.000 deg Focal Surface# Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano At infinity 1 Lens 125.83945 0.57735 Glass 1.56384 60.7 −4.99728 2 2.52696 1.482023 3 Lens 29.12695 3.276371 Plastic 1.65 21.4 35.7892 4 12.81628 0.049817 5 Ape.Stop Plano 0.4 6 Lens 3 13.78383 1.259894 Glass 2.001 29.13 3.06725 7−3.79913 0.166918 8 Lens 4 −3.45617 0.3 Plastic 1.65 21.4 −2.97038 94.61165 0.107861 10 Lens 5 6.40049 1.72256 Plastic 1.565 58 4.6518 11−4.0469 0.05 12 Lens 6 −10.8812 0.646965 Glass 1.497 81.61 22.8248 13−5.66991 0.7 14 IR-bandstop Plano 0.85 BK_7 1.517 64.13 filter 15 Plano4.410239 16 Image plane Plano Reference wavelength (d-line) = 555 nmAs for the parameters of the aspheric surfaces of the seventhEmbodiment, reference is made to Table 14.

TABLE 14 Aspheric Coefficients Surface # 3 4 6 7 8 9 10 k 5.42118634.081963 0.000000E+00 0.000000E+00 −0.130464 −2.829009 −1.354227 A47.44705E−04 7.24190E−03 0.000000E+00 0.000000E+00 −2.18182E−05−1.61987E−03 −6.88971E−04 A6 1.31143E−04 −2.40196E−03 0.000000E+000.000000E+00 2.84075E−04 −4.35256E−05 3.20238E−04 A8 −7.41900E−062.98968E−03 0.000000E+00 0.000000E+00 1.65500E−04 3.73337E−055.74429E−06 A10 1.61914E−06 −1.06068E−03 0.000000E+00 0.000000E+006.05544E−06 −2.34181E−06 8.38341E−07 Surface # 11 12 13 k −0.78750.000000E+00 0.000000E+00 A4 9.61923E−04 0.000000E+00 0.000000E+00 A63.06516E−04 0.000000E+00 0.000000E+00 A8 −4.07384E−06 0.000000E+000.000000E+00 A10 1.36567E−05 0.000000E+00 0.000000E+00

In the seventh Embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 13 and Table 14.

Seventh embodiment (Primary reference wavelength: 555 nm) ETP1 ETP2 ETP3ETP4 ETP5 ETP6 0.658 3.271 1.185 0.412 1.633 0.628 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 1.140 0.998 0.940 1.374 0.948 0.971ETL EBL EIN EIR PIR EIN/ETL 15.991  6.000 9.992 0.739 0.700 0.625SETP/EIN EIR/PIR SETP STP SETP/STP BL 0.779 1.056 7.787 7.783 1.0015.960 ED12 ED23 ED34 ED45 ED56 EBL/BL 1.417 0.447 0.161 0.095 0.084 1.0067 SED SIN SED/SIN ED12/ED23 ED23/ED34 ED34/ED45 2.204 2.257 0.9773.171 2.774 1.695 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45 ED56/IN56ED45/ED56 0.956 0.993 0.965 0.881 1.687 1.127 | f/f1 | | f/f2 | | f/f3 || f/f4 | | f/f5 | | f/f6 |  0.74714  0.10432  1.21727  1.25697  0.80263 0.16358 Σ PPR/ TP4/(IN34 + Σ PPR Σ NPR | Σ NPR | IN12/f IN56/f TP4 +IN45)  2.28780  2.00411  1.14156  0.39693  0.01339  0.52194 | f1/f2 | |f2/f3 | (TP1 + IN12)/TP2 (TP6 + IN56)/TP5  0.13963  11.66817 0.628550.40461 HOS InTL HOS/HOI InS/HOS ODT % TDT %  16.00000  10.03980 4.00000  0.66341 −38.1161  25.1423 HVT51 HVT52 HVT61 HVT62 HVT62/HOIHVT62/HOS 0    0     0.00000  0.00000  0.00000  0.00000 TP2/TP3 TP3/TP4InRS61 InRS62 | InRS61 |/TP6 | InRS62 |/TP6  2.60052  4.19963  −0.29936 −0.64630  0.46271  0.99898 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.88 0.84  0.84  0.74  0.64  0.66  MTFI0 MTFI3 MTFI7 0.83  0.81  0.77 

The following contents may be deduced from Table 13 and Table 14.

Related inflection point values of seventh embodiment (Primary referencewavelength: 555 nm) HIF411 1.7754 HIF411/HOI 0.4438 SGI411 −0.4588|0.4588|/(.4588HO| + TP4) 0.6046 HIF521 1.8025 HIF521/HOI 0.4506 SGI521−0.3806 |SGI5216/(|SGI5216/(It) 0.1810

The Eight Embodiment (Embodiment 8)

Please refer to FIG. 8A, FIG. 8B, FIGS. 8C, and 8D. FIG. 8A is aschematic view of the optical image capturing system according to theeighth Embodiment of the present application, FIG. 8B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the eighth Embodiment of the presentapplication, FIG. 8C is a characteristic diagram of modulation transferof a visible light according to the eighth embodiment of the presentapplication and FIG. 8D is a characteristic diagram of modulationtransfer of infrared rays according to the eighth embodiment of thepresent application. As shown in FIG. 8A, in order from an object sideto an image side, the optical image capturing system includes anaperture stop 800, a first lens element 810, a second lens element 820,a third lens element 830, a fourth lens element 840, a fifth lenselement 850, a sixth lens element 860, an IR-bandstop filter 880, animage plane 890, and an image sensing device 892.

The first lens element 810 has positive refractive power and it is madeof plastic material. The first lens element 810 has a convex object-sidesurface 812 and a concave image-side surface 814, both of theobject-side surface 812 and the image-side surface 814 are aspheric, andthe image-side surface 814 has an inflection point.

The second lens element 820 has negative refractive power and it is madeof plastic material. The second lens element 820 has a concaveobject-side surface 822 and a concave image-side surface 824, and bothof the object-side surface 822 and the image-side surface 824 areaspheric. The image-side surface 824 has two inflection points.

The third lens element 830 has negative refractive power and it is madeof plastic material. The third lens element 830 has a convex object-sidesurface 832 and a concave image-side surface 834, and both of theobject-side surface 832 and the image-side surface 834 are aspheric. Theobject-side surface 832 and the image-side surface 834 both have aninflection point.

The fourth lens element 840 has positive refractive power and it is madeof plastic material. The fourth lens element 840 has a concaveobject-side surface 842 and a convex image-side surface 844, and both ofthe object-side surface 842 and the image-side surface 844 are aspheric.The object-side surface 842 has three inflection points.

The fifth lens element 850 has positive refractive power and it is madeof plastic material. The fifth lens element 850 has a convex object-sidesurface 852 and a convex image-side surface 854, and both of theobject-side surface 852 and the image-side surface 854 are aspheric. Theobject-side surface 852 has three inflection points and the image-sidesurface 854 has an inflection point.

The sixth lens element 860 has negative refractive power and it is madeof plastic material. The sixth lens element 860 has a concaveobject-side surface 862 and a concave image-side surface 864. Theobject-side surface 862 has two inflection points and the image-sidesurface 864 has an inflection point. Hereby, the back focal length isreduced to miniaturize the lens element effectively. In addition, theangle of incident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 880 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 860 and the image plane 890.

In the optical image capturing system of the eighth Embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=12.785 mm andf5/ΣPP=0.10. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the eighth Embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=−112.117 mm andf6/ΣNP=0.009. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 15 and Table 16.

The detailed data of the optical image capturing system of the eighthEmbodiment is as shown in Table 15.

TABLE 15 Data of the optical image capturing system f = 3.213 mm; f/HEP= 2.4; HAF = 50.015 deg Focal Surface# Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano At infinity 1 Shading Plano0.000 sheet 2 Ape. Stop Plano −0.108 3 Lens 1 2.117380565 0.267 Plastic1.565 58.00 6.003 4 5.351202213 0.632 5 Lens 2 −70.37596785 0.230Plastic 1.517 21.40 −11.326 6 8.30936549 0.050 7 Lens 3 7.3331718650.705 Plastic 1.565 58.00 −99.749 8 6.265499794 0.180 9 Lens 4−71.32533363 0.832 Plastic 1.565 58.00 5.508 10 −3.003657909 0.050 11Lens 5 3.397431079 0.688 Plastic 1.583 30.20 1.274 12 −0.886432266 0.05013 Lens 6 −3.715425702 0.342 Plastic 1.650 21.40 −1.042 14 0.8676236370.700 15 IR-bandstop Plano 0.200 1.517 64.13 filter 16 Plano 0.407 17Image plane Plano Reference wavelength (d-line) = 555 nm; shieldposition: clear aperture (CA) of the first plano = 0.640 mmAs for the parameters of the aspheric surfaces of the eighth Embodiment,reference is made to Table 16.

TABLE 16 Aspheric Coefficients Surface # 3 4 5 6 7 8 9 k −1.486403E+002.003790E+01 −4.783682E+01 −2.902431E+01 −5.000000E+01 −5.000000E+01−5.000000E+01 A4 2.043654E−02 −2.642626E−02 −6.237485E−02 −4.896336E−02−7.363667E−02 −5.443257E−02 3.105497E−02 A6 −2.231403E−04 −4.147746E−02−8.137705E−02 −1.981368E−02 1.494245E−02 1.263891E−04 −1.532514E−02 A8−1.387235E−02 2.901026E−02 4.589961E−02 3.312952E−03 6.252296E−03−9.655324E−03 −6.443603E−04 A10 −3.431740E−02 −9.512960E−02−5.485574E−02 5.634445E−03 −2.226544E−03 1.318692E−03 4.321089E−04 A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface # 10 11 1213 14 k 8.520005E−01 −5.000000E+01 −4.524978E+00 −5.000000E+01−4.286435E+00 A4 −6.786287E−03 −9.520247E−02 −4.666187E−02 5.856863E−03−2.635938E−02 A6 6.693976E−03 −5.507560E−05 3.849227E−03 2.442214E−033.694093E−03 A8 8.220809E−04 1.932773E−03 1.041053E−03 −2.201034E−03−1.355873E−04 A10 −2.798394E−04 3.346274E−04 4.713339E−06 −1.065215E−04−5.321575E−05 A12 0.000000E+00 1.125736E−05 −2.834871E−06 1.227641E−046.838440E−06 A14 0.000000E+00 −1.671951E−05 −2.293810E−06 −1.181115E−05−2.530792E−07

In the eighth Embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 15 and Table 16.

Eighth embodiment (Primary reference wavelength: 555 nm) ETP1 ETP2 ETP3ETP4 ETP5 ETP6 0.203 0.263 0.710 0.760 0.479 0.556 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.759 1.142 1.008 0.914 0.696 1.628ETL EBL EIN EIR PIR EIN/ETL 5.234 1.134 4.100 0.527 0.700 0.783 SETP/EINEIR/PIR SETP STP SETP/STP BL 0.725 0.753 2.971 3.064 0.970 1.304 ED12ED23 ED34 ED45 ED56 EBL/BL 0.580 0.050 0.161 0.150 0.188  0.8696 SED SINSED/SIN 1.129 0.962 1.173 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45ED56/IN56 0.917 1.005 0.896 2.997 3.756 | f/f1 | | f/f2 | | f/f3 | |f/f4 | | f/f5 | | f/f6 |  0.53529  0.28371  0.03221  0.58335  2.52139 3.08263 Σ PPR/ TP4/(IN34 + Σ PPR Σ NPR | Σ NPR | IN12/f IN56/f TP4 +IN45)  6.72266  0.84594  7.94700  0.19680  0.01556  0.78362 | f1/f2 | |f2/f3 | (TP1 + IN12)/TP2 (TP6 + IN56)/TP5  0.53001  0.11354 3.909470.56888 HOS InTL HOS/HOI InS/HOS ODT % TDT %  5.33002  4.02576  1.36178 0.97981  1.92371  1.09084 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 0.67483 0     0.00000  2.23965  0.57222  0.42020 TP2/TP3 TP3/TP4 InRS61InRS62 | InRS61 |/TP6 | InRS62 |/TP6  0.32631  0.84713   −0.74088  −0.06065  2.16896  0.17755 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.9 0.85  0.8  0.77  0.63  0.51  MTFI0 MTFI3 MTFI7 0.45  0.03  0.22 

The following contents may be deduced from Table 15 and Table 16.

Related inflection point values of eighth Embodiment (Primary referencewavelength: 555 nm) HIF121 0.57452 HIF121/HOI 0.14679 SGI121 0.02858|SGI1218/(|SGI1218/(It) 0.09675 HIF221 0.40206 HIF221/HOI 0.10272 SGI2210.00821 |SGI2211/(|SGI2211/(It) 0.03448 HIF222 1.11769 HIF222/HOI0.28556 SGI222 −0.02234 |SGI2223/(|SGI2223/(It) 0.08853 HIF311 0.37391HIF311/HOI 0.09553 SGI311 0.00785 |.00785|/(00785HO| + TP3) 0.01102HIF321 0.42061 HIF321/HOI 0.10746 SGI321 0.01170 |SGI3210/(|SGI3210/(It)0.01633 HIF411 0.19878 HIF411/HOI 0.05079 SGI411 −0.00023|0.0002|/(.00023O| + TP4) 0.00028 HIF412 0.87349 HIF412/HOI 0.22317SGI412 0.00583 |.00583|/(00583HO| + TP4) 0.00695 HIF413 1.87638HIF413/HOI 0.47940 SGI413 −0.17360 |0.I413|/(.I4130O| + TP4) 0.17263HIF511 0.36373 HIF511/HOI 0.09293 SGI511 0.015644 |.01564|/(015644O| +TP5) 0.02222 HIF512 1.7159  HIF512/HOI 0.43840 SGI512 −0.446747|0.4467/(.446747| + TP5) 0.39358 HIF513 1.93653 HIF513/HOI 0.49477SGI513 −0.638544 |0.6385|/(|SGI513| + TP5) 0.48124 HIF521 1.54767HIF521/HOI 0.39542 SGI521 −0.792114 |SGI5211/(|SGI5211/(It) 0.53505HIF611 0.82168 HIF611/HOI 0.20993 SGI611 −0.060958 |0.0609/(.060958| +TP6) 0.15143 HIF612 0.98146 HIF612/HOI 0.25076 SGI612 −0.07785|0.0778/(.077612| + TP6) 0.18561 HIF621 0.79476 HIF621/HOI 0.20306SGI621 0.238143 |SGI6214/(|SGI6214/(It) 0.41079

The above-mentioned descriptions represent merely the exemplaryembodiment of the present disclosure, without any intention to limit thescope of the present disclosure thereto. Various equivalent changes,alternations or modifications based on the claims of present disclosureare all consequently viewed as being embraced by the scope of thepresent disclosure.

What is claimed is:
 1. An optical image capturing system, from an objectside to an image side, comprising: a first lens element with refractivepower; a second lens element with refractive power; a third lens elementwith refractive power; a fourth lens element with refractive power; afifth lens element with refractive power; a sixth lens element withrefractive power; and an image plane; wherein the optical imagecapturing system consists of six lens elements with refractive power, amaximum height for image formation on the image plane perpendicular tothe optical axis in the optical image capturing system is denoted byHOI, at least one of the first through sixth lens elements has positiverefractive power, an object-side surface and an image-side surface ofthe sixth lens element are aspheric, focal lengths of the first throughsixth lens elements are f1, f2, f3, f4, f5 and f6 respectively, a focallength of the optical image capturing system is f, an entrance pupildiameter of the optical image capturing system is HEP, a distance on anoptical axis from an axial point on an object-side surface of the firstlens element to an axial point on the image plane is HOS, thicknesses inparallel with an optical axis of the first through sixth lens elementsat height ½ HEP respectively are ETP1, ETP2, ETP3, ETP4, ETP5 and ETP6,a sum of ETP1 to ETP6 described above is SETP, thicknesses of the firstthrough sixth lens elements on the optical axis respectively are TP1,TP2, TP3, TP4, TP5 and TP6, a sum of TP1 to TP6 described above is STP,and the following relations are satisfied: 1.2≤f/HEP≤10.0 and0.5≤SETP/STP<1; wherein a half of maximum view angle of the opticalimage capturing system is HAF, and the following relation is satisfied:1.19≤|tan(HAF)|≤6.0.
 2. The optical image capturing system of claim 1,wherein a horizontal distance in parallel with the optical axis from acoordinate point on the object-side surface of the first lens element atheight ½ HEP to the image plane is ETL, a horizontal distance inparallel with the optical axis from a coordinate point on theobject-side surface of the first lens element at height ½ HEP to acoordinate point on the image-side surface of the sixth lens element atheight ½ HEP is EIN, and the following relation is satisfied:0.2≤EIN/ETL<1.
 3. The optical image capturing system of claim 2, whereinthe thicknesses in parallel with the optical axis of the first throughsixth lens elements at height ½ HEP respectively are ETP1, ETP2, ETP3,ETP4, ETP5 and ETP6, the sum of ETP1 to ETP6 described above is SETP,and the following relation is satisfied: 0.3≤SETP/EIN<1.
 4. The opticalimage capturing system of claim 1, wherein the optical image capturingsystem comprises a light filtration element, the light filtrationelement is located between the sixth lens element and the image plane, adistance in parallel with the optical axis from a coordinate point onthe image-side surface of the sixth lens element at height ½ HEP to thelight filtration element is EIR, a distance in parallel with the opticalaxis from an axial point on the image-side surface of the sixth lenselement to the light filtration element is PIR, and the followingrelation is satisfied: 0.1≤EIR/PIR≤1.1.
 5. The optical image capturingsystem of claim 1, wherein an object-side surface or an image-sidesurface of at least one lens element among the six lens elements has atleast one inflection point.
 6. The optical image capturing system ofclaim 1, wherein contrast transfer rates of modulation transfer withspace frequencies of 55 cycles/mm (MTF values) of a visible light at theoptical axis on the image plane, 0.3 HOI and 0.7 HOI are respectivelydenoted by MTFE0, MTFE3 and MTFE7, and the following relations aresatisfied: MTFE0≥0.2, MTFE3≥0.01 and MTFE7≥0.01.
 7. The optical imagecapturing system of claim 1, wherein a horizontal distance in parallelwith the optical axis from a coordinate point on the image-side surfaceof the sixth lens element at height ½ HEP to the image plane is EBL, ahorizontal distance in parallel with the optical axis from an axialpoint on the image-side surface of the sixth lens element to the imageplane is BL, and the following relation is satisfied: 0.1≤EBL/BL<0.1. 8.The optical image capturing system of claim 1, further comprising anaperture stop, a distance from the aperture stop to the image plane onthe optical axis is InS, an image sensing device is disposed on theimage plane, and the following relations are satisfied: 0.1≤InS/HOS≤1.1and 0≤HIF/HOI≤0.9.
 9. An optical image capturing system, from an objectside to an image side, comprising: a first lens element with negativerefractive power; a second lens element with refractive power; a thirdlens element with refractive power; a fourth lens element withrefractive power; a fifth lens element with refractive power; a sixthlens element with refractive power; and an image plane; wherein theoptical image capturing system consists of six lens elements withrefractive power and at least one lens element of the six lens elementsis made of glass material, a maximum height for image formation on theimage plane perpendicular to the optical axis in the optical imagecapturing system is denoted by HOI, at least one of the second throughsixth lens elements has positive refractive power, focal lengths of thefirst through sixth lens elements are f1, f2, f3, f4, f5 and f6respectively, a focal length of the optical image capturing system is f,an entrance pupil diameter of the optical image capturing system is HEP,a distance on an optical axis from an axial point on an object-sidesurface of the first lens element to an axial point on the image planeis HOS, a horizontal distance in parallel with the optical axis from acoordinate point on the object-side surface of the first lens element atheight ½ HEP to the image plane is ETL, a horizontal distance inparallel with the optical axis from a coordinate point on theobject-side surface of the first lens element at height ½ HEP to acoordinate point on the image-side surface of the sixth lens element atheight ½ HEP is EIN, and the following relations are satisfied:1.2≤f/HEP≤10.0 and 0.2≤EIN/ETL<1; wherein a half of maximum view angleof the optical image capturing system is HAF, and the following relationis satisfied: 1.19≤|tan(HAF)|≤6.0.
 10. The optical image capturingsystem of claim 9, wherein a horizontal distance in parallel with theoptical axis from a coordinate point on the image-side surface of thefifth lens element at height ½ HEP to a coordinate point on theobject-side surface of the sixth lens element at height ½ HEP is ED56, adistance from the fifth lens element to the sixth lens element on theoptical axis is IN56, and the following relation is satisfied:0<ED56/IN56≤50.
 11. The optical image capturing system of claim 9,wherein a horizontal distance in parallel with the optical axis from acoordinate point on the image-side surface of the first lens element atheight ½ HEP to a coordinate point on the object-side surface of thesecond lens element at height ½ HEP is ED12, a distance from the firstlens element to the second lens element on the optical axis is IN12, andthe following relation is satisfied: 0<ED12/IN12<10.
 12. The opticalimage capturing system of claim 9, wherein a thickness in parallel withthe optical axis of the second lens element at height ½ HEP is ETP2, athickness of the second lens element on the optical axis is TP2, and thefollowing relation is satisfied: 0<ETP2/TP2≤3.
 13. The optical imagecapturing system of claim 9, wherein a thickness in parallel with theoptical axis of the fifth lens element at height ½ HEP is ETP5, athickness of the fifth lens element on the optical axis is TP5, and thefollowing relation is satisfied: 0<ETP5/TP5≤3.
 14. The optical imagecapturing system of claim 9, wherein a thickness in parallel with theoptical axis of the sixth lens element at height ½ HEP is ETP6, athickness of the sixth lens element on the optical axis is TP6, and thefollowing relation is satisfied: 0<ETP6/TP6≤5.
 15. The optical imagecapturing system of claim 9, wherein a distance from the first lenselement to the second lens element on the optical axis is IN12, and thefollowing relation is satisfied: 0<IN12/f≤60.
 16. The optical imagecapturing system of claim 9, wherein contrast transfer rates ofmodulation transfer with spatial frequencies of 55 cycles/mm of aninfrared operation wavelength 850 nm at the optical axis on the imageplane, 0.3 HOI and 0.7 HOI are respectively denoted by MTFI0, MTFI3 andMTFI7, and the following relations are satisfied: MTFI0≥0.01, MTFI3≥0.01and MTFI7≥0.01.
 17. The optical image capturing system of claim 9,wherein contrast transfer rates of modulation transfer with spacefrequencies of 110 cycles/mm of a visible light at the optical axis onthe image plane, 0.3 HOI and 0.7 HOI are respectively denoted by MTFQ0,MTFQ3 and MTFQ7, and the following relations are satisfied: MTFQ0≥0.2,MTFQ3≥0.01 and MTFQ7≥0.01.
 18. The optical image capturing system ofclaim 9, wherein at least one of the first, the second, the third, thefourth, the fifth and the sixth lens elements is a light filtrationelement with a wavelength of less than 500 nm.
 19. An optical imagecapturing system, from an object side to an image side, comprising: afirst lens element with negative refractive power; a second lens elementwith refractive power; a third lens element with refractive power; afourth lens element with refractive power; a fifth lens element withrefractive power; a sixth lens element with refractive power, and animage plane; wherein the optical image capturing system consists of sixlens elements with refractive power and at least three lens elements ofthe six lens elements are made of glass material, a maximum height forimage formation on the image plane perpendicular to the optical axis inthe optical image capturing system is denoted by HOI, and at least onelens element among the first through sixth lens elements respectivelyhas at least one inflection point on at least one surface thereof, anobject-side surface and an image-side surface of at least one lenselement of the six lens elements are aspheric, and focal lengths of thefirst through sixth lens elements are f1, f2, f3, f4, f5 and f6respectively, a focal length of the optical image capturing system is f,an entrance pupil diameter of the optical image capturing system is HEP,a half of maximum view angle of the optical image capturing system isHAF, a distance on an optical axis from an axial point on an object-sidesurface of the first lens element to an axial point on the image planeis HOS, a horizontal distance in parallel with the optical axis from acoordinate point on the object-side surface of the first lens element atheight ½ HEP to the image plane is ETL, a horizontal distance inparallel with the optical axis from a coordinate point on theobject-side surface of the first lens element at height ½ HEP to acoordinate point on the image-side surface of the sixth lens element atheight ½ HEP is EIN, and the following relations are satisfied:1.2≤f/HEP≤10.0, 1.19≤|tan(HAF)|≤6.0, and 0.2≤EIN/ETL<1.
 20. The opticalimage capturing system of claim 19, wherein a horizontal distance inparallel with the optical axis from a coordinate point on the image-sidesurface of the sixth lens element at height ½ HEP to the image plane isEBL, a horizontal distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theimage plane is BL, and the following relation is satisfied:0.1≤EBL/BL≤1.1.
 21. The optical image capturing system of claim 20,wherein a horizontal distance in parallel with the optical axis from acoordinate point on the image-side surface of the fifth lens element atheight ½ HEP to a coordinate point on the object-side surface of thesixth lens element at height ½ HEP is ED56, a distance from the fifthlens element to the sixth lens element on the optical axis is IN56, andthe following relation is satisfied: 0<ED56/IN56≤50.
 22. The opticalimage capturing system of claim 19, wherein a distance from the fifthlens element to the sixth lens element on the optical axis is IN56, andthe following relation is satisfied: 0<IN56/f≤5.0.
 23. The optical imagecapturing system of claim 22, wherein the optical image capturing systemsatisfies the following relation: 0 mm<HOS≤50 mm.
 24. The optical imagecapturing system of claim 22, further comprising an aperture stop, animage sensing device and a driving module, the image sensing device isdisposed on the image plane, a distance from the aperture stop to theimage plane on the optical axis is InS, the driving module and the sixlens elements couple to each other and shifts are produced for the sixlens elements, and the following relation is satisfied: 0.1≤InS/HOS≤1.1.